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Top 20 Most Read Articles

June 2010

The 20 articles with the most full-text downloads during the month, in descending order.


Three-dimensional imaging of pore structures inside low-κ dielectrics

Huolin L. Xin, Peter Ercius, Kevin J. Hughes, James R. Engstrom, and David A. Muller

Appl. Phys. Lett. 96, 223108 (2010); http://dx.doi.org/10.1063/1.3442496 (3 pages)

Online Publication Date: 2 June 2010

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The three-dimensional reconstruction of a porous low-dielectric constant film (κ = 2.5), resolving pores as small as 1 nm, was achieved using annular dark-field scanning transmission electron tomography, enabling quantitative measurements of the pore morphologies and size distribution. Most large pores were elliptical. Together with log-normal pore-size distribution, this suggests pore coalescence during the material’s growth. Ellipsometric porosimetry indicates a high degree of interconnectivity between pores. Tomography shows the material exhibits little large-scale pore connectivity, thus placing an upper limit on the size of the interconnections at below 1 nm. Systematic errors in the tomographic and ellipsometric size distributions appear to be largely complementary.
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77.55.Bh Low-permittivity dielectric films
61.46.-w Structure of nanoscale materials
61.43.Gt Powders, porous materials

Emission color control from blue to red with nanocolumn diameter of InGaN/GaN nanocolumn arrays grown on same substrate

Hiroto Sekiguchi, Katsumi Kishino, and Akihiko Kikuchi

Appl. Phys. Lett. 96, 231104 (2010); http://dx.doi.org/10.1063/1.3443734 (3 pages)

Online Publication Date: 7 June 2010

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A novel technology for controlling the In composition of InGaN quantum wells on the same wafer was developed, which paved the way for the monolithic integration of three-primary-color nano-light-emitting diodes. In the experiment, InGaN/GaN multiple quantum well nanocolumn arrays with nanocolumn diameters from 137 to 270 nm were prepared on the same substrate with the Ti-mask selective area growth by rf-plasma-assisted molecular beam epitaxy. The emission color changed from blue to red (from 479 to 632 nm in wavelength) with increasing nanocolumn diameter. The emission color change mechanism was clearly explained by the beam shadow effect of the neighboring nanocolumns.
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78.67.De Quantum wells
78.55.Cr III-V semiconductors
85.35.Be Quantum well devices (quantum dots, quantum wires, etc.)
85.60.Jb Light-emitting devices
81.16.-c Methods of micro- and nanofabrication and processing

Optically pumped ultraviolet lasing from nitride nanopillars at room temperature

Rui Chen, H. D. Sun, T. Wang, K. N. Hui, and H. W. Choi

Appl. Phys. Lett. 96, 241101 (2010); http://dx.doi.org/10.1063/1.3449576 (3 pages)

Online Publication Date: 14 June 2010

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A vertical cavity structure composing of an in situ grown bottom AlxGa1−xN/AlyGa1−yN distributed Bragg reflector and a top SiO2/HfO2 dielectric mirror for ultraviolet (UV) emission has been demonstrated. Close-packed nanopillars with diameters of around 500 nm have been achieved by the route of nanosphere lithography combined with inductively-coupled plasma etching. Optically-pumped UV lasing at a wavelength of 343.7 nm (3.608 eV) was observed at room temperature, with a threshold excitation density of 0.52 MW/cm2. The mechanism of the lasing action is discussed in detail. Our investigation indicates promising possibilities in nitride-based resonant cavity devices, particularly toward realizing the UV nitride-based vertical-cavity surface-emitting laser.
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42.55.Px Semiconductor lasers; laser diodes
42.60.By Design of specific laser systems
42.72.Bj Visible and ultraviolet sources
42.60.Da Resonators, cavities, amplifiers, arrays, and rings

Nonuniformity of a planar polarizer for spin-transfer-induced vortex oscillations at zero field

A. V. Khvalkovskiy, J. Grollier, N. Locatelli, Ya. V. Gorbunov, K. A. Zvezdin, and V. Cros

Appl. Phys. Lett. 96, 212507 (2010); http://dx.doi.org/10.1063/1.3441405 (3 pages)

Online Publication Date: 28 May 2010

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We discuss a possible mechanism of the spin-transfer-induced oscillations of a vortex in the free layer of spin-valve nanostructures, in which the polarizer layer has a planar magnetization. We demonstrate that if such planar polarizer is essentially nonuniform, steady gyrotropic vortex motion with large amplitude can be excited. The best excitation efficiency is obtained for a circular magnetization distribution in the polarizer. In this configuration, the conditions for the onset of the oscillations depend on the vortex chirality but not on the direction of its core.
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85.75.-d Magnetoelectronics; spintronics: devices exploiting spin polarized transport or integrated magnetic fields
75.70.Cn Magnetic properties of interfaces (multilayers, superlattices, heterostructures)

Low efficiency droop in blue-green m-plane InGaN/GaN light emitting diodes

Shih-Chun Ling, Tien-Chang Lu, Shih-Pang Chang, Jun-Rong Chen, Hao-Chung Kuo, and Shing-Chung Wang

Appl. Phys. Lett. 96, 231101 (2010); http://dx.doi.org/10.1063/1.3449557 (3 pages)

Online Publication Date: 7 June 2010

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We investigated the electroluminescence and relatively external quantum efficiency (EQE) of m-plane InGaN/GaN light emitting diodes (LEDs) emitting at 480 nm to elucidate the droop behaviors in nitride-based LEDs. With increasing the injection current density to 100 A/cm2, the m-plane LEDs exhibit only 13% efficiency droop, whereas conventional c-plane LEDs suffer from efficiency droop at very low injection current density and the EQE of c-plane LEDs decrease to as little as 50% of its maximum value. Our simulation models show that in m-plane LEDs the absence of polarization fields manifest not only the hole distribution more uniform among the wells but also the reduction in electron overflow out of electron blocking layer. These results suggest that the nonuniform distribution of holes and electron leakage current due to strong polarization fields are responsible for the relatively significant efficiency droop of conventional c-plane LEDs.
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85.60.Jb Light-emitting devices

Comment on “Guided modes in graphene waveguides” [ Appl. Phys. Lett. 94, 212105 (2009) ]

Cesar E. P. Villegas and Marcos R. S. Tavares

Appl. Phys. Lett. 96, 186101 (2010); http://dx.doi.org/10.1063/1.3425716 (2 pages)

Online Publication Date: 5 May 2010

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Abstract Unavailable
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84.40.Az Waveguides, transmission lines, striplines

Response to “Comment on ‘Guided modes in graphene waveguides’” [ Appl. Phys. Lett. 96, 186101 (2010) ]

Ying He, Fan-Ming Zhang, and Xi Chen

Appl. Phys. Lett. 96, 186102 (2010); http://dx.doi.org/10.1063/1.3425717 (2 pages)

Online Publication Date: 5 May 2010

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Abstract Unavailable
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42.79.Gn Optical waveguides and couplers
73.20.At Surface states, band structure, electron density of states

Metal-cavity surface-emitting microlaser at room temperature

Chien-Yao Lu, Shu-Wei Chang, Shun Lien Chuang, Tim D. Germann, and Dieter Bimberg

Appl. Phys. Lett. 96, 251101 (2010); http://dx.doi.org/10.1063/1.3455316 (3 pages)

Online Publication Date: 21 June 2010

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We propose and realize a substrate-free metal-cavity surface-emitting microlaser with both top and sidewall metal and a bottom distributed Bragg reflector as the cavity structure. The transfer-matrix method is used to design the laser structure based on the round-trip resonance condition inside the cavity. The laser is 2.0 μm in diameter and 2.5 μm in height, and operates at room temperature with continuous-wave mode. Flip-bonding the device to a silicon substrate with a conductive metal provides efficient heat removal. A high characteristic temperature about 425 K is observed from 10 to 27 °C.
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42.55.Px Semiconductor lasers; laser diodes
42.60.By Design of specific laser systems
42.60.Da Resonators, cavities, amplifiers, arrays, and rings
42.55.Sa Microcavity and microdisk lasers
42.79.Bh Lenses, prisms and mirrors

Optical gain in carbon nanotubes

Etienne Gaufrès, Nicolas Izard, Xavier Le Roux, Delphine Marris-Morini, Saïd Kazaoui, Eric Cassan, and Laurent Vivien

Appl. Phys. Lett. 96, 231105 (2010); http://dx.doi.org/10.1063/1.3443634 (3 pages)

Online Publication Date: 8 June 2010

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Semiconducting single-wall carbon nanotubes (s-SWNTs) have proved to be promising material for nanophotonics and optoelectronics. Due to the possibility of tuning their direct band gap and controlling excitonic recombinations in the near-infrared wavelength range, s-SWNT can be used as efficient light emitters. We report the first experimental demonstration of room temperature intrinsic optical gain as high as 190 cm−1 at a wavelength of 1.3 μm in a thin film doped with s-SWNT. These results constitute a significant milestone toward the development of laser sources based on carbon nanotubes for future high performance integrated circuits.
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71.35.-y Excitons and related phenomena

Enhancement of light extraction from GaN-based green light-emitting diodes using selective area photonic crystal

Ja-Yeon Kim, Min-Ki Kwon, Seong-Ju Park, Sang Hoon Kim, and Ki-Dong Lee

Appl. Phys. Lett. 96, 251103 (2010); http://dx.doi.org/10.1063/1.3454240 (3 pages)

Online Publication Date: 22 June 2010

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We report the development of a GaN-based green light-emitting diode (LED) with a selective area photonic crystal (SPC) structure, which was formed outside the p-bonding electrode on p-GaN. As a result, the optical output power of LEDs with SPC was enhanced by 78% compared to that without PC. In addition, the forward voltage, series resistance, and leakage current of LEDs with SPC were remarkably improved. These results show that the light extraction efficiency of green LEDs can be greatly increased using the SPC structure, with no degradation of electrical properties.
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85.60.Jb Light-emitting devices

Comment on “Influence of random roughness on cantilever curvature sensitivity” [ Appl. Phys. Lett. 96, 041912 (2010) ]

Yan Wang, Jörg Weissmüller, and Huiling Duan

Appl. Phys. Lett. 96, 226101 (2010); http://dx.doi.org/10.1063/1.3442493 (1 page)

Online Publication Date: 1 June 2010

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Abstract Unavailable
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68.35.B- Structure of clean surfaces (and surface reconstruction)
05.20.-y Classical statistical mechanics
46.25.Cc Theoretical studies

Scatterer induced mode splitting in poly(dimethylsiloxane) coated microresonators

Lina He, Sahin Kaya Ozdemir, Jiangang Zhu, and Lan Yang

Appl. Phys. Lett. 96, 221101 (2010); http://dx.doi.org/10.1063/1.3435480 (3 pages)

Online Publication Date: 1 June 2010

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We investigate scatterer induced mode splitting in a composite microtoroidal resonator (Q ∼ 106) fabricated by coating a silica microtoroid (Q ∼ 107) with a thin poly(dimethylsiloxane) layer. We show that the two split modes in both coated and uncoated silica microtoroids respond in the same way to the changes in the environmental temperature. This provides a self-referencing scheme which is robust to temperature perturbations. Together with the versatile functionalities of polymer materials, mode splitting in polymer and polymer coated microresonators offers an attractive sensing platform that is robust to thermal noise.
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68.55.-a Thin film structure and morphology
85.85.+j Micro- and nano-electromechanical systems (MEMS/NEMS) and devices

Strong coupling in a quantum dot micropillar system under electrical current injection

C. Kistner, K. Morgener, S. Reitzenstein, C. Schneider, S. Höfling, L. Worschech, A. Forchel, P. Yao, and S. Hughes

Appl. Phys. Lett. 96, 221102 (2010); http://dx.doi.org/10.1063/1.3442912 (3 pages)

Online Publication Date: 1 June 2010

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Integrating In0.3Ga0.7As quantum dots (QDs) featuring a high oscillator strength into a high quality electrically contacted micropillar cavity enabled us to realize strong coupling under electrical carrier injection. In the micropillar cavity with a quality factor of 10 000 and a diameter of 1.9 μm, a vacuum Rabi splitting of 108 μeV was observed when an electrically excited QD exciton was tuned through resonance with the fundamental cavity mode by varying the temperature.
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73.63.Kv Quantum dots
78.67.Hc Quantum dots
73.20.Mf Collective excitations (including excitons, polarons, plasmons and other charge-density excitations)
73.21.La Quantum dots

Fast reset and suppressing spontaneous emission of a superconducting qubit

M. D. Reed, B. R. Johnson, A. A. Houck, L. DiCarlo, J. M. Chow, D. I. Schuster, L. Frunzio, and R. J. Schoelkopf

Appl. Phys. Lett. 96, 203110 (2010); http://dx.doi.org/10.1063/1.3435463 (3 pages)

Online Publication Date: 21 May 2010

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Spontaneous emission through a coupled cavity can be a significant decay channel for qubits in circuit quantum electrodynamics. We present a circuit design that effectively eliminates spontaneous emission due to the Purcell effect while maintaining strong coupling to a low-Q cavity. Excellent agreement over a wide range in frequency is found between measured qubit relaxation times and the predictions of a circuit model. Using fast (nanosecond time-scale) flux biasing of the qubit, we demonstrate in situ control of qubit lifetime over a factor of 50. We realize qubit reset with 99.9% fidelity in 120 ns.
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03.67.Lx Quantum computation architectures and implementations
03.67.Hk Quantum communication
42.50.Pq Cavity quantum electrodynamics; micromasers

Response to “Comment on ‘Influence of random roughness on cantilever curvature sensitivity’ ” [ Appl. Phys. Lett. 96, 226101 (2010) ]

O. Ergincan, G. Palasantzas, and B. J. Kooi

Appl. Phys. Lett. 96, 226102 (2010); http://dx.doi.org/10.1063/1.3442494 (1 page)

Online Publication Date: 1 June 2010

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Abstract Unavailable
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99.10.-x Errata and other corrections
06.30.Bp Spatial dimensions (e.g., position, lengths, volume, angles, and displacements)
75.30.Kz Magnetic phase boundaries (including classical and quantum magnetic transitions, metamagnetism, etc.)

Theory of electroluminescence intensity and insights into recombination in thin film solar cells

Gregory Brown, Vladimir Faifer, Ben Cardozo, Eugene Bykov, and Miguel Contreras

Appl. Phys. Lett. 96, 222102 (2010); http://dx.doi.org/10.1063/1.3443637 (3 pages)

Online Publication Date: 1 June 2010

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Equations describing the electroluminescence (EL) intensity as a function of material properties are derived for thin film solar cells and experimentally validated using Cu(In,Ga)Se2 solar cells. EL intensity at constant voltage is controlled by the electronic properties of the neutral bulk even when the diode current is controlled by recombination in the space charge region. Using a combination of techniques, it is found that recombination in the quasineutral bulk does not correlate with recombination in the space charge region. Differences between EL measurements on thin film cells and crystalline silicon cells are discussed including the effects of secondary barriers.
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88.40.jn Thin film Cu-based I-III-VI2 solar cells
85.30.De Semiconductor-device characterization, design, and modeling

Comment on “Ferroelectricity in glycine picrate: An astonishing observation in a centrosymmetric crystal” [ Appl. Phys. Lett. 95, 252902 (2009) ]

Zbigniew Tylczyński and Maciej Wiesner

Appl. Phys. Lett. 96, 126101 (2010); http://dx.doi.org/10.1063/1.3372622 (1 page)

Online Publication Date: 22 March 2010

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Abstract Unavailable
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77.80.-e Ferroelectricity and antiferroelectricity
77.22.Ej Polarization and depolarization
77.80.Dj Domain structure; hysteresis
77.22.Ch Permittivity (dielectric function)
61.72.-y Defects and impurities in crystals; microstructure
81.40.Np Fatigue, corrosion fatigue, embrittlement, cracking, fracture, and failure

Rare frustration of optical supercontinuum generation

D. R. Solli, C. Ropers, and B. Jalali

Appl. Phys. Lett. 96, 151108 (2010); http://dx.doi.org/10.1063/1.3374860 (3 pages)

Online Publication Date: 14 April 2010

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Recent work has shown that optical rogue waves, large bandwidth fluctuations following heavy-tailed statistics, can arise during spectral broadening by stochastic enhancement of nonlinearity. Here, we report the observation of a different form of extreme fluctuations in supercontinuum pulse trains: Pulses of unusually small spectral bandwidth following left-skewed heavy-tailed statistics. Displaying a pulse evolution strongly varying from that of large extremes in supercontinuum, these rogue events appear when spectral broadening is frustrated by competition between presolitonic features within the modulation-instability band. This suppression effect can also be externally induced with a weak control pulse.
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42.65.Re Ultrafast processes; optical pulse generation and pulse compression
02.50.Ey Stochastic processes

Comment on “Carbon nanowalls as material for electrochemical transducers” [ Appl. Phys. Lett. 95, 014104 (2009) ]

Ali Eftekhari

Appl. Phys. Lett. 96, 126102 (2010); http://dx.doi.org/10.1063/1.3357437 (2 pages)

Online Publication Date: 23 March 2010

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Abstract Unavailable
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82.45.Yz Nanostructured materials in electrochemistry
61.46.-w Structure of nanoscale materials
82.65.+r Surface and interface chemistry; heterogeneous catalysis at surfaces
61.43.Dq Amorphous semiconductors, metals, and alloys
82.45.Fk Electrodes

Comment on “Direct measurement of minority carriers diffusion length using Kelvin probe force microscopy” [ Appl. Phys. Lett. 75, 2435 (1999) ]

Mohammed Shahriar Sabuktagin

Appl. Phys. Lett. 96, 216101 (2010); http://dx.doi.org/10.1063/1.3431743 (1 page)

Online Publication Date: 24 May 2010

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Abstract Unavailable
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73.40.Lq Other semiconductor-to-semiconductor contacts, p-n junctions, and heterojunctions
72.20.Jv Charge carriers: generation, recombination, lifetime, and trapping
73.25.+i Surface conductivity and carrier phenomena
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