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3 Oct 2011

Volume 99, Issue 14, Articles (14xxxx)

Issue Cover Spotlight Figure

Appl. Phys. Lett. 99, 141901 (2011); http://dx.doi.org/10.1063/1.3644948 (3 pages)

G. Kozlowski, P. Zaumseil, M. A. Schubert, Y. Yamamoto, J. Bauer, J. Matejova, T. Schulli, B. Tillack, and T. Schroeder
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Generating intense ultrashort radiation by reflecting an ultrashort laser pulse from a thin target

Wenmin Zhang (张文敏) and M. Y. Yu (郁明阳)

Appl. Phys. Lett. 99, 141501 (2011); http://dx.doi.org/10.1063/1.3645630 (3 pages) | Cited 1 time

Online Publication Date: 3 October 2011

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Particle-in-cell simulation and analytical modeling demonstrate that the reflection of a single-cycle light pulse from a thin target can produce an ultrashort ultraintense electromagnetic field.
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52.38.Kd Laser-plasma acceleration of electrons and ions
52.65.Rr Particle-in-cell method

Density evolution measurement of hydrogen plasma in capillary discharge by spectroscopy and interferometry methods

D. G. Jang, M. S. Kim, I. H. Nam, H. S. Uhm, and H. Suk

Appl. Phys. Lett. 99, 141502 (2011); http://dx.doi.org/10.1063/1.3643134 (3 pages) | Cited 3 times

Online Publication Date: 5 October 2011

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Plasma density is one of the most important parameters for laser wakefield acceleration using a gas-filled capillary waveguide. We measured the evolving hydrogen plasma densities in capillary discharge by using two different diagnostics methods at the same time, i.e., the Stark-effect-based spectroscopy and the transverse interferometry methods. It was found that there is a rather large difference between two methods and the phenomenon is explained in view of self-absorption. The correlation was obtained and the result is quite useful for capillary-plasma-based laser wakefield acceleration research.
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52.70.Kz Optical (ultraviolet, visible, infrared) measurements
52.80.Tn Other gas discharges
29.20.Ej Linear accelerators
52.25.-b Plasma properties
52.38.Kd Laser-plasma acceleration of electrons and ions

Microwave diagnostics of femtosecond laser-generated plasma filaments

J. Papeer, C. Mitchell, J. Penano, Y. Ehrlich, P. Sprangle, and A. Zigler

Appl. Phys. Lett. 99, 141503 (2011); http://dx.doi.org/10.1063/1.3643478 (3 pages) | Cited 2 times

Online Publication Date: 5 October 2011

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We present a simple non-intrusive experimental method allowing a complete single shot temporal measurement of laser produced plasma filament conductivity. The method is based on filament interaction with low intensity microwave radiation in a rectangular waveguide. The suggested diagnostics allow a complete single shot temporal analysis of filament plasma decay with resolution better than 0.3 ns and high spatial resolution along the filament. The experimental results are compared to numerical simulations, and an initial electron density of 7 × 1016 cm−3 and decay time of 3 ns are obtained.
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52.38.Hb Self-focussing, channeling, and filamentation in plasmas
52.25.Fi Transport properties
52.70.Gw Radio-frequency and microwave measurements
42.65.Jx Beam trapping, self-focusing and defocusing; self-phase modulation
42.65.Re Ultrafast processes; optical pulse generation and pulse compression

Ionization wave propagation on a micro cavity plasma array

Alexander Wollny, Torben Hemke, Markus Gebhardt, Ralf Peter Brinkmann, Henrik Boettner, Jörg Winter, Volker Schulz-von der Gathen, Zhongmin Xiong, Mark J. Kushner, and Thomas Mussenbrock

Appl. Phys. Lett. 99, 141504 (2011); http://dx.doi.org/10.1063/1.3647978 (3 pages) | Cited 1 time

Online Publication Date: 6 October 2011

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Microcavity plasma arrays of inverse pyramidal cavities fabricated on p-Si wafers act as localized dielectric barrier discharges. When operated at atmospheric pressure in argon and excited with high voltage at 10 kHz, a strong interaction between individual cavities is observed leading to wave-like optical emission propagating along the surface of the array. This phenomenon is numerically investigated. The computed ionization wave propagates with a speed of 5 km/s, which agrees well with experiments. The wave propagation is due to the sequential drift of electrons followed by drift of ions between cavities seeded by photoemission of electrons by the plasma in adjacent cavities.
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52.30.-q Plasma dynamics and flow
52.25.Os Emission, absorption, and scattering of electromagnetic radiation
52.50.Dg Plasma sources
52.65.-y Plasma simulation
52.80.Dy Low-field and Townsend discharges
52.80.Hc Glow; corona
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