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7 Jun 2010

Volume 96, Issue 23, Articles (23xxxx)

Issue Cover Spotlight Figure

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

Hiroto Sekiguchi, Katsumi Kishino, and Akihiko Kikuchi
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The functionalization of graphene using electron-beam generated plasmas

M. Baraket, S. G. Walton, E. H. Lock, J. T. Robinson, and F. K. Perkins

Appl. Phys. Lett. 96, 231501 (2010); http://dx.doi.org/10.1063/1.3436556 (3 pages) | Cited 13 times

Online Publication Date: 8 June 2010

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A plasmas-based, reversible functionalization of graphene is discussed. Using electron-beam produced plasmas, oxygen and fluorine functionalities have been added by changing the processing gas mixtures from Ar/O2 to Ar/SF6, respectively. The reversibility of the functionalization was investigated by annealing the samples. The chemical composition and structural changes were studied by x-ray photoelectron spectroscopy and Raman spectroscopy.
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78.67.Wj Optical properties of graphene
64.75.Cd Phase equilibria of fluid mixtures, including gases, hydrates, etc.
78.30.Na Fullerenes and related materials
82.80.Pv Electron spectroscopy (X-ray photoelectron (XPS), Auger electron spectroscopy (AES), etc.)
81.40.Gh Other heat and thermomechanical treatments
79.60.-i Photoemission and photoelectron spectra

Prediction of atmospheric pressure glow discharge in dielectric-barrier system

Xiaoxi Duan, Feng He, and Jiting Ouyang

Appl. Phys. Lett. 96, 231502 (2010); http://dx.doi.org/10.1063/1.3453451 (3 pages) | Cited 1 time

Online Publication Date: 11 June 2010

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A one-dimensional fluid model was used to investigate the breakdown mechanism and discharge mode in dielectric-barrier system. The results show that the dielectric barrier discharge mode depends strongly on the gas property (i.e., the electron multiplication). The atmospheric pressure dielectric barrier glow discharge could only be achieved in a gas (e.g., noble gas) in which the first Townsend ionization coefficient is sufficiently small and the electron multiplication does not rise up rapidly with the electric field, while could not be sustained in the gas (e.g., N2 and O2) in which the electron multiplication is sensitive to the field.
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52.80.Hc Glow; corona
52.80.Dy Low-field and Townsend discharges

Desktop megawatt superradiant free-electron laser at terahertz frequencies

Yen-Chieh Huang (黃衍介)

Appl. Phys. Lett. 96, 231503 (2010); http://dx.doi.org/10.1063/1.3447928 (3 pages) | Cited 2 times

Online Publication Date: 11 June 2010

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I present a theoretical and simulation study of a desktop, megawatt (MW), terahertz (THz) superradiance free-electron laser (FEL) driven by a THz-pulse-train photoinjector. With nominal electron parameters from a THz-pulse-train photoinjector, this superradiant FEL is capable of generating more than 5 MW power at THz frequencies from a half-meter, single-pass undulator. Tapering the undulator to a length of 1.5 m can further increase the FEL output power to nearly 15 MW.
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41.60.Cr Free-electron lasers
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