• Volume/Page
  • Keyword
  • DOI
  • Citation
  • Advanced
   
 
 
 

Flickr Twitter iResearch App Facebook

Top 20 Most Read Articles

November 2009

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


Self-assembled nanodielectrics and silicon nanomembranes for low voltage, flexible transistors, and logic gates on plastic substrates

Hoon-Sik Kim, Sang Min Won, Young-Geun Ha, Jong-Hyun Ahn, Antonio Facchetti, Tobin J. Marks, and John A. Rogers

Appl. Phys. Lett. 95, 183504 (2009); http://dx.doi.org/10.1063/1.3256223 (3 pages)

Online Publication Date: 4 November 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
This letter reports the fabrication and electrical characterization of mechanically flexible and low operating voltage transistors and logic gates (NOT, NAND, and NOR gates) using printed silicon nanomembranes and self-assembled nanodielectrics on thin plastic substrates. The transistors exhibit effective linear mobilities of ∼ 680 cm2/V s, on/off ratios >107, gate leakage current densities <2.8×10−7 A/cm2, and subthreshold slopes ∼ 120 mV/decade. The inverters show voltage gains as high as 4.8. Simple digital logic gates (NAND and NOR gates) demonstrate the possible application of this materials combination in digital integrated circuits.
Show PACS
84.30.Sk Pulse and digital circuits
85.30.Tv Field effect devices
81.05.Cy Elemental semiconductors
81.07.-b Nanoscale materials and structures: fabrication and characterization

Optical nanorod antennas as dispersive one-dimensional Fabry–Pérot resonators for surface plasmons

Ertugrul Cubukcu and Federico Capasso

Appl. Phys. Lett. 95, 201101 (2009); http://dx.doi.org/10.1063/1.3262947 (3 pages)

Online Publication Date: 16 November 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
Resonant optical nanoantennas exhibit a different length scaling due to the surface plasmons compared to their radio frequency counterparts. In this letter, we address this difference by calculating the wavelength-dependent effective mode index neff for a cylindrical one-dimensional gold nanowire waveguide. Our results show that nanorod optical antennas act as dispersive and lossy Fabry–Pérot resonators for surface plasmons.
Show PACS
42.82.-m Integrated optics
42.79.Gn Optical waveguides and couplers

Energetic disorder limits energy transfer in semiconductor nanocrystal–DNA–dye conjugates

Klaus Becker, Andrey L. Rogach, Jochen Feldmann, Dmitri V. Talapin, and John M. Lupton

Appl. Phys. Lett. 95, 143101 (2009); http://dx.doi.org/10.1063/1.3242015 (3 pages)

Online Publication Date: 5 October 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
We demonstrate the influence of spectral linewidths of individual donor-acceptor couples on energy transfer efficiency in semiconductor nanocrystal–DNA–organic dye conjugates. Temperature-dependent single molecule and ensemble spectroscopy data are analyzed using the Förster theory within the macroscopic and microscopic approaches. The results obtained evidence on the importance of the spectral overlap between emission of a single donor and absorption of a single acceptor in its close vicinity, which determines the microscopic resonance and transfer efficiency between individual neighbors. This realization poses important implications on the applicability of ensemble spectral overlap for the analysis of distance dependencies of nanoscopic objects.
Show PACS
78.67.Bf Nanocrystals, nanoparticles, and nanoclusters
87.14.gk DNA
78.55.-m Photoluminescence, properties and materials

A pathway to p-type wide-band-gap semiconductors

Anderson Janotti, Eric Snow, and Chris G. Van de Walle

Appl. Phys. Lett. 95, 172109 (2009); http://dx.doi.org/10.1063/1.3247890 (3 pages)

Online Publication Date: 30 October 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
Based on first-principles calculations we devise an alternative approach to p-type doping in AlN, ZnO, and ZnMgO. Instead of searching for acceptors on the left of the host atoms in the Periodic Table, we propose to search on the far right. We find that F placed at interstitial sites in AlN, ZnO, and ZnMgO acts as a shallow acceptor, leaving a hole in an effective-mass state near the valence-band maximum. We investigate the stability of F impurities and propose a procedure to selectively introduce F in the interstitial lattice sites of the above wide-band-gap semiconductors.
Show PACS
61.72.uj III-V and II-VI semiconductors
71.15.-m Methods of electronic structure calculations
71.18.+y Fermi surface: calculations and measurements; effective mass, g factor
71.20.Nr Semiconductor compounds
61.72.jj Interstitials

Blue light-emitting diodes with a roughened backside fabricated by wet etching

Chia-Feng Lin, Chun-Min Lin, Kuei-Ting Chen, Wan-Chun Huang, Ming-Shiou Lin, Jing-Jie Dai, Ren-Hao Jiang, Yu-Chieh Huang, and Chung-Ying Chang

Appl. Phys. Lett. 95, 201102 (2009); http://dx.doi.org/10.1063/1.3262968 (3 pages)

Online Publication Date: 16 November 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
The InGaN-based light-emitting diodes (LEDs) with a roughened patterned backside on the N-face GaN surface were fabricated through a crystallographic etching process to increase light-extraction efficiency. After laser decomposition, laser scribing, and a lateral crystallographic wet etching process at the GaN/Al2O3 interface, stable crystallographic etching planes were formed as the GaN {10math} planes that included an angle with the top GaN (0001) plane measured at 58°. The GaN buffer layer acted as the sacrificial layer for the laser decomposition process and the lateral wet etching process with a 26 μm/min etching rate. The LED with the inverted pyramidal N-face GaN surface close to the GaN/Al2O3 interface has a larger light-scattering process than the conventional LED. The light-output power of the LED with the backside roughened surface had a 47% enhancement when measured in LED chip form.
Show PACS
85.60.Jb Light-emitting devices

Scalable arrays of rf Paul traps in degenerate Si

J. Britton, D. Leibfried, J. A. Beall, R. B. Blakestad, J. H. Wesenberg, and D. J. Wineland

Appl. Phys. Lett. 95, 173102 (2009); http://dx.doi.org/10.1063/1.3254188 (3 pages)

Online Publication Date: 26 October 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
We report techniques for the fabrication of multizone linear radio frequency Paul traps that exploit the machinability and electrical conductivity of degenerate silicon. The approach was tested by trapping and laser cooling 24Mg+ ions in the two following trap geometries: a single-zone two-layer trap and a multizone surface-electrode trap. From the measured ion motional heating rate we determine an electric field spectral density at the ion’s position of approximately 1×10−10 (V/m)2⋅Hz−1 at ωz/2π = 1.125 MHz when the ion lies 40 μm above the trap surface. One application of these devices is controlled manipulation of atomic ion qubits, the basis of one form of quantum information processing.
Show PACS
72.20.Fr Low-field transport and mobility; piezoresistance
72.80.Cw Elemental semiconductors
03.67.Lx Quantum computation architectures and implementations
07.10.Cm Micromechanical devices and systems
85.85.+j Micro- and nano-electromechanical systems (MEMS/NEMS) and devices

Transfer of graphene layers grown on SiC wafers to other substrates and their integration into field effect transistors

Sakulsuk Unarunotai, Yuya Murata, Cesar E. Chialvo, Hoon-sik Kim, Scott MacLaren, Nadya Mason, Ivan Petrov, and John A. Rogers

Appl. Phys. Lett. 95, 202101 (2009); http://dx.doi.org/10.1063/1.3263942 (3 pages)

Online Publication Date: 16 November 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
This letter presents a simple method for transferring epitaxial sheets of graphene on silicon carbide to other substrates. The graphene was grown on the (0001) face of 6H-SiC by thermal annealing at 1550 °C in a hydrogen atmosphere. Transfer was accomplished using a peeling process with a bilayer film of gold/polyimide, to yield graphene with square millimeters of coverage on the target substrate. Raman spectroscopy provided evidence that the transferred material is single layer. Back gated field-effect transistors fabricated on oxidized silicon substrates with Cr/Au as source-drain electrodes exhibited ambipolar characteristics with hole mobilities of ∼ 100 cm2/V-s, and negligible influence of resistance at the contacts.
Show PACS
85.30.Tv Field effect devices
73.40.Cg Contact resistance, contact potential
78.30.Na Fullerenes and related materials
73.63.-b Electronic transport in nanoscale materials and structures
78.67.Wj Optical properties of graphene
61.72.Cc Kinetics of defect formation and annealing

Oxidation of silver electrodes induces transition from conventional to inverted photovoltaic characteristics in polymer solar cells

Jong Bok Kim, Chang Su Kim, Youn Sang Kim, and Yueh-Lin Loo

Appl. Phys. Lett. 95, 183301 (2009); http://dx.doi.org/10.1063/1.3257361 (3 pages)

Online Publication Date: 3 November 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
Oxidation of silver top electrodes in polymer solar cells induces the devices to exhibit a transition from conventional to inverted photovoltaic characteristics. As silver oxidizes, its work function increases from 4.3 to 5.0 eV. The silver top electrode thus reverts from collecting electrons to collecting holes during device operation. We have quantified the extent of this transformation and find it to be correlated with the rate of silver oxidation, which we can influence by altering the annealing sequence of the polymer photoactive layer, ultimately varying the grain size of silver in the top electrode.
Show PACS
72.40.+w Photoconduction and photovoltaic effects
73.30.+y Surface double layers, Schottky barriers, and work functions
81.40.Ef Cold working, work hardening; annealing, post-deformation annealing, quenching, tempering recovery, and crystallization

Design of graphene electronic devices using nanoribbons of different widths

G. G. Naumis, M. Terrones, H. Terrones, and L. M. Gaggero-Sager

Appl. Phys. Lett. 95, 182104 (2009); http://dx.doi.org/10.1063/1.3257731 (3 pages)

Online Publication Date: 5 November 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
We present a simple design of a field effect transistor based on graphene nanoribbons, taking advantage of the metallic and semiconductor nature of nanoribbons with different widths. Such device could be constructed by using lithography techniques. The conductance of the proposed device is obtained by using the Kubo formula, assuming a strong damping due to the substrate and imperfections of the lattice. By removing the control electrodes, the design could also be used as an electrical resistance.
Show PACS
85.30.Tv Field effect devices
81.16.Nd Micro- and nanolithography

Improving optical performance of inverted organic solar cells by microcavity effect

Yongbing Long (龙拥兵)

Appl. Phys. Lett. 95, 193301 (2009); http://dx.doi.org/10.1063/1.3262967 (3 pages)

Online Publication Date: 11 November 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
Optical simulations have been performed to investigate the performance of inverted organic solar cells with metal-mirror microcavity structure formed by central active layer sandwiched between semitransparent silver (Ag) cathode and thick Ag anode. Compared to nearly optimized noncavity devices with indium tin oxide cathode, the total absorbed photons (TAPs) in a 70 nm-thick active layer for cavity devices can be improved by 16.3% due to microcavity effect. Furthermore, an improvement of over 10% in TAPs can be obtained when thin Ag layer is optimized to be 10–16 nm thick, indicating thin Ag layer is a good choice as transparent electrode material.
Show PACS
88.40.jr Organic photovoltaics

A tunable few electron triple quantum dot

L. Gaudreau, A. Kam, G. Granger, S. A. Studenikin, P. Zawadzki, and A. S. Sachrajda

Appl. Phys. Lett. 95, 193101 (2009); http://dx.doi.org/10.1063/1.3258663 (3 pages)

Online Publication Date: 9 November 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
In this paper, we report on a tunable few electron lateral triple quantum dot design. The quantum dot potentials are arranged in series. The device is aimed at studies of triple quantum dot properties where knowing the exact number of electrons is important as well as quantum information applications involving electron spin qubits. We demonstrate tuning strategies for achieving required resonant conditions such as quadruple points where all three quantum dots are on resonance. We find that in such a device resonant conditions at specific configurations are accompanied by complex charge transfer behavior.
Show PACS
73.63.Kv Quantum dots
68.65.Hb Quantum dots (patterned in quantum wells)

Nanowire-quantum-dot solar cells and the influence of nanowire length on the charge collection efficiency

Kurtis S. Leschkies, Alan G. Jacobs, David J. Norris, and Eray S. Aydil

Appl. Phys. Lett. 95, 193103 (2009); http://dx.doi.org/10.1063/1.3258490 (3 pages)

Online Publication Date: 10 November 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
External quantum efficiency in solar cells based on junctions between PbSe quantum dots (QDs) and thin ZnO films is increased by replacing the ZnO films with a vertically oriented array of single-crystalline ZnO nanowires, and infiltrating this array with colloidal QDs. When illuminated with 100 mW/cm2 of simulated solar light, QD-nanowire solar cells exhibited power conversion efficiencies approaching 2%, approximately three times higher than that achieved with thin-film ZnO devices constructed with the same amount of QDs. Significant photocurrent and power conversion improvement with increasing nanowire length is consistent with higher exciton and charge collection efficiencies.
Show PACS
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)
73.50.Pz Photoconduction and photovoltaic effects
68.55.-a Thin film structure and morphology
82.70.Dd Colloids

Electroluminescence induced by photoluminescence excitation in GaInN/GaN light-emitting diodes

Martin F. Schubert, Qi Dai, Jiuru Xu, Jong Kyu Kim, and E. Fred Schubert

Appl. Phys. Lett. 95, 191105 (2009); http://dx.doi.org/10.1063/1.3258488 (3 pages)

Online Publication Date: 10 November 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
Optical emission resulting from 405 nm selective photoexcitation of carriers in the GaInN/GaN quantum well (QW) active region of a light-emitting diode reveals two recombination channels. The first recombination channel is the recombination of photoexcited carriers in the GaInN QWs. The second recombination channel is formed by carriers that leak out of the GaInN QW active region, self-bias the device in forward direction, induce a forward current, and subsequently recombine in the GaInN active region in a spatially distributed manner. The results indicate dynamic carrier transport involving active, confinement, and contact regions of the device.
Show PACS
85.60.Jb Light-emitting devices
81.07.St Quantum wells
78.66.Fd III-V semiconductors
81.05.Ea III-V semiconductors

Electrically tunable terahertz quantum-cascade laser with a heterogeneous active region

Suraj P. Khanna, Mohammed Salih, Paul Dean, A. Giles Davies, and Edmund H. Linfield

Appl. Phys. Lett. 95, 181101 (2009); http://dx.doi.org/10.1063/1.3253714 (3 pages)

Online Publication Date: 2 November 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
We demonstrate experimentally a terahertz frequency quantum-cascade laser which can be tuned electronically, in a step-wise manner from typically 3.07 to 3.40 THz, by changing the applied electric field across the device. To achieve this, the gallium growth rate was successively reduced during growth of the active region from +6% to −4% of its nominal 1 μm/h operating value. This produced a heterogeneous active region, comprising 23 sections of different lasing units stacked together. With a single-metal surface-plasmon waveguide configuration, the devices operated in pulsed mode, up to a temperature of 81 K, and gave peak powers of ∼ 8 mW.
Show PACS
42.55.Px Semiconductor lasers; laser diodes
42.60.Fc Modulation, tuning, and mode locking
42.79.Gn Optical waveguides and couplers
42.60.Jf Beam characteristics: profile, intensity, and power; spatial pattern formation

Direct near-field optical investigation of phase-change medium in blue-ray recordable and erasable disk

Jen-You Chu, Shen-Chuan Lo, Shu-Chen Chen, You-Chia Chang, and Juen-Kai Wang

Appl. Phys. Lett. 95, 103105 (2009); http://dx.doi.org/10.1063/1.3222901 (3 pages)

Online Publication Date: 9 September 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
The authors report a direct examination of recorded marks in blue-ray recordable and erasable disks with scattering-type scanning near-field optical microscopy. The optical contrasts of the crystalline and amorphous regions of the phase-change layer match with the prediction based on their optical constants. The determined spatial optical variation in the recorded marks reflects the intensity profile of the recording laser beam. The identified nanometer-sized optical features are shown to correspond to 10 nm-sized crystalline domains within the amorphous recorded marks. The revealed near-field signatures show a potential influence on the carrier-to-noise ratio of this optical storage medium.
Show PACS
42.79.Vb Optical storage systems, optical disks

Two-state competition in 1.3 μm multilayer InAs/InGaAs quantum dot lasers

Q. Cao, S. F. Yoon, C. Z. Tong, C. Y. Ngo, C. Y. Liu, R. Wang, and H. X. Zhao

Appl. Phys. Lett. 95, 191101 (2009); http://dx.doi.org/10.1063/1.3259659 (3 pages)

Online Publication Date: 9 November 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
The competition of ground state (GS) and excited state (ES) is investigated from the as-grown and thermally annealed 1.3 μm ten-layer p-doped InAs/GaAs quantum dot (QD) lasers. The modal gain competition between GS and ES are measured and analyzed around the ES threshold characteristics. Our results show that two-state competition is more significant in devices with short cavity length operating at high temperature. By comparing the as-grown and annealed devices, we demonstrate enhanced GS and suppressed ES lasing from the QD laser annealed at 600 °C for 15 s.
Show PACS
42.55.Px Semiconductor lasers; laser diodes
42.60.By Design of specific laser systems
42.79.Wc Optical coatings
42.60.Da Resonators, cavities, amplifiers, arrays, and rings
42.60.Jf Beam characteristics: profile, intensity, and power; spatial pattern formation

ZnO/TiO2 nanonetwork as efficient photoanode in excitonic solar cells

A. Vomiero, I. Concina, M. M. Natile, E. Comini, G. Faglia, M. Ferroni, I. Kholmanov, and G. Sberveglieri

Appl. Phys. Lett. 95, 193104 (2009); http://dx.doi.org/10.1063/1.3257370 (3 pages)

Online Publication Date: 11 November 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
An innovative nanonetwork composed of TiO2 nanoparticles and single-crystalline ZnO nanowires is demonstrated as efficient photoanode in excitonic solar cells. Such architecture benefits of the capability of high sensitizer loading offered by the nanoparticles and of the direct conduction path for electrons guaranteed by the nanowires. The combination of these features leads to improved light absorption, electron photogeneration, and charge collection. The nanonetwork was implemented in a dye-sensitized solar-cell architecture demonstrating threefold enhancement of the efficiency with respect to a nanowire photoanode of the same thickness. Cell efficiency of 1.6% was obtained in 1.5 μm thick nanonetwork.
Show PACS
88.40.hj Efficiency and performance of solar cells
88.40.jm Thin film III-V and II-VI based solar cells

Photocurrent enhancement in polymer:fullerene bulk heterojunction solar cells doped with a phosphorescent molecule

Barry P. Rand, Claudio Girotto, Alexander Mityashin, Afshin Hadipour, Jan Genoe, and Paul Heremans

Appl. Phys. Lett. 95, 173304 (2009); http://dx.doi.org/10.1063/1.3257383 (3 pages)

Online Publication Date: 30 October 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
We demonstrate photocurrent enhancement of up to 20% in polymer:fullerene bulk heterojunction photovoltaic cells via the incorporation of a phosphorescent dopant, without degradation in the open-circuit voltage or fill factor of the device. The enhancement is shown to originate from multiple sources. First, the phosphor is able to populate the long-lived triplet state of the polymer, leading to longer diffusion length and a larger polymer contribution. Also, there is direct absorption on the dopant leading to enhanced spectral coverage. Finally, the dopant acts as a donor site and therefore increases the fullerene signal.
Show PACS
66.30.H- Self-diffusion and ionic conduction in nonmetals
72.40.+w Photoconduction and photovoltaic effects
81.05.Lg Polymers and plastics; rubber; synthetic and natural fibers; organometallic and organic materials

Vertically aligned ZnO nanostructures grown on graphene layers

Yong-Jin Kim, Jae-Hyun Lee, and Gyu-Chul Yi

Appl. Phys. Lett. 95, 213101 (2009); http://dx.doi.org/10.1063/1.3266836 (3 pages)

Online Publication Date: 24 November 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
We report the vertical growth of ZnO nanostructures on graphene layers and their photoluminescence (PL) characteristics. ZnO nanostructures were grown vertically on the graphene layers using catalyst-free metal-organic vapor-phase epitaxy. The surface morphology of the ZnO nanostructures on the graphene layers depended strongly on the growth temperature. Further, interesting growth behavior leading to the formation of aligned ZnO nanoneedles in a row and vertically aligned nanowalls was also observed and explained in terms of enhanced nucleation on graphene step edges and kinks. Additionally, the optical characteristics and carbon incorporation into ZnO were investigated using variable-temperature PL spectroscopy.
Show PACS
81.07.-b Nanoscale materials and structures: fabrication and characterization
61.46.-w Structure of nanoscale materials
68.35.bg Semiconductors
81.15.Kk Vapor phase epitaxy; growth from vapor phase
81.15.Gh Chemical vapor deposition (including plasma-enhanced CVD, MOCVD, ALD, etc.)
78.55.Et II-VI semiconductors
78.67.-n Optical properties of low-dimensional, mesoscopic, and nanoscale materials and structures

Giant tunneling magnetoresistance up to 330% at room temperature in sputter deposited Co2FeAl/MgO/CoFe magnetic tunnel junctions

Wenhong Wang, Hiroaki Sukegawa, Rong Shan, Seiji Mitani, and Koichiro Inomata

Appl. Phys. Lett. 95, 182502 (2009); http://dx.doi.org/10.1063/1.3258069 (3 pages)

Online Publication Date: 3 November 2009

Full Text: Read Online (HTML) | Download PDF

Show Abstract
Magnetoresistance ratio up to 330% at room temperature (700% at 10 K) has been obtained in a spin-valve-type magnetic tunnel junction (MTJ) consisting of a full-Heusler alloy Co2FeAl electrode and a MgO tunnel barrier fabricated on a single crystal MgO (001) substrate by sputtering method. The output voltage of the MTJ at one-half of the zero-bias value was found to be as high as 425 mV, which is the largest reported to date in MTJs using Heusler alloy electrodes. The present finding suggests that Co2FeAl may be one of the most promising candidates for future spintronics devices applications.
Show PACS
75.47.De Giant magnetoresistance
73.50.Jt Galvanomagnetic and other magnetotransport effects (including thermomagnetic effects)
81.15.Cd Deposition by sputtering
75.70.Cn Magnetic properties of interfaces (multilayers, superlattices, heterostructures)
Close
Google Calendar
ADVERTISEMENT

close