001     151970
005     20210129213629.0
024 7 _ |a 10.1117/12.2017254
|2 doi
024 7 _ |a WOS:000323544600039
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037 _ _ |a FZJ-2014-01797
100 1 _ |a Gopal, Amrutha
|0 P:(DE-HGF)0
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|e Corresponding Author
111 2 _ |a SPIE Optics + Optoelectronics
|c Prague
|d 2013-04-15 - 2013-04-18
|w Czech Republic
245 _ _ |a 700μJ THz pulses from a laser-driven particle accelerator
260 _ _ |a Washington, DC
|c 2013
|b Society of Photo-Optical Instrumentation Engineers (SPIE)
295 1 0 |a SPIE Proceedings, Volume 8779, Laser Acceleration of Electrons, Protons, and Ions II; and Medical Applications of Laser-Generated Beams of Particles II; and Harnessing Relativistic Plasma Waves III
300 _ _ |a 123-150
336 7 _ |a Contribution to a conference proceedings
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336 7 _ |a Contribution to a book
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336 7 _ |a Conference Paper
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336 7 _ |a CONFERENCE_PAPER
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336 7 _ |a INPROCEEDINGS
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520 _ _ |a Here we report a laser plasma-driven source of T-rays with the highest pulse energy ever recorded in a laboratory. T-rays are emitted from therear surface of a solid target in the non-collinear direction at incident laser intensities ~ 10^19 W/cm^2. Pulse energy measurements reported T-ray pulses with peak energies no less than 700 μJ. Temporal measurements using a single-shot electro-optic method showed the presence of sub-picosecond T-ray pulseswith 570 fs duration, thus rendering the peak-power of the source higher even than that of state-of-the-art synchrotrons. A conversion efficiencyof higher than 10^-3 and an average power of 7 mW makes it the most efficient compact and powerful THz source known today. Spectral analysis revealed the presences of frequencies ranging from 0.1 - 133 THz, while most of the energy is localised in the low frequency region. The dependence of T-ray yield on incident laser energy is linear and shows no signs of saturation. The spatial distribution of the recorded T-rays indicates that most of the T-rays are emitted in the non-collinear direction from the rear-surface of a solid target and the contribution in the forward direction is very small. 2D particle-in-cellsimulations show the presence of transient current at the target rear surface.
536 _ _ |a 411 - Computational Science and Mathematical Methods (POF2-411)
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536 _ _ |a EMMI - Helmholtz-Allianz 'Kosmische Materie im Labor', Extreme Matter Institute (HGF-IVF-HA-216)
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588 _ _ |a Dataset connected to CrossRef Conference
700 1 _ |a May, Torsten
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700 1 _ |a Singh, Pushkar
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700 1 _ |a Herzer, Sven
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700 1 _ |a Ziegler, Wolfgang
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700 1 _ |a Paulus, Gerhard G.
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700 1 _ |a Schmidt, Albrecht
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700 1 _ |a Reinhard, Andreas
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700 1 _ |a Dillner, Ulrich
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700 1 _ |a Meyer, Hans-Georg
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700 1 _ |a Karmakar, Anupam
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700 1 _ |a Brömmel, Dirk
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700 1 _ |a Gibbon, Paul
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773 _ _ |a 10.1117/12.2017254
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910 1 _ |a Forschungszentrum Jülich GmbH
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913 2 _ |a DE-HGF
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914 1 _ |y 2014
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