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23 Jun 2008

Volume 92, Issue 25, Articles (25xxxx)

Issue Cover Spotlight Figure

Appl. Phys. Lett. 92, 254102 (2008); http://dx.doi.org/10.1063/1.2945893 (3 pages)

M. Trinker, S. Groth, S. Haslinger, S. Manz, T. Betz, S. Schneider, I. Bar-Joseph, T. Schumm, and J. Schmiedmayer
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Efficient 13.5 nm extreme ultraviolet emission from Sn plasma irradiated by a long CO2 laser pulse

Y. Tao, M. S. Tillack, K. L. Sequoia, R. A. Burdt, S. Yuspeh, and F. Najmabadi

Appl. Phys. Lett. 92, 251501 (2008); http://dx.doi.org/10.1063/1.2951595 (3 pages) | Cited 20 times

Online Publication Date: 23 June 2008

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The effect of pulse duration on in-band (2% bandwidth) conversion efficiency (CE) from a CO2 laser to 13.5 nm extreme ultraviolet (EUV) light was investigated for Sn plasma. It was found that high in-band CE, 2.6%, is consistently obtained using a CO2 laser with pulse durations from 25 to 110 ns. Employing a long pulse, for example, 110 ns, in a CO2 laser system used in an EUV lithography source could make the system significantly more efficient, simpler, and cheaper as compared to that using a short pulse of 25 ns or shorter.
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52.50.Jm Plasma production and heating by laser beams (laser-foil, laser-cluster, etc.)
42.72.Bj Visible and ultraviolet sources
42.65.Re Ultrafast processes; optical pulse generation and pulse compression

Hard x-ray generation by low energy, tightly focused laser pulses

K. Takano, K. Nemoto, T. Nayuki, Y. Oishi, T. Fujii, A. Zhidkov, E. Hotta, M. Todoriki, and S. Hasegawa

Appl. Phys. Lett. 92, 251502 (2008); http://dx.doi.org/10.1063/1.2945283 (3 pages) | Cited 2 times

Online Publication Date: 24 June 2008

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The interaction of λ2 laser pulses with plasma is studied to scale the high-field physics from high power laser systems to low-energy, high-repetition-rate lasers. For this purpose, 20 mJ, 40 fs Ti:sapphire laser pulses were focused in a spot of 2.2×2.3 μm2 with a maximum intensity of I ∼ 1019W/cm2. Efficient generations of energetic electrons ( ∼ 1 MeV) and hard x-rays with energies of over 100 keV were obtained by irradiating the low-energy, tightly focused laser pulses on a massive Cu target.
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52.38.Ph X-ray, γ-ray, and particle generation
52.38.Kd Laser-plasma acceleration of electrons and ions

Pulsed corona discharge for oxidation of gaseous elemental mercury

Kyung Bo Ko, Youngchul Byun, Moohyun Cho, Won Namkung, Ian P. Hamilton, Dong Nam Shin, Dong Jun Koh, and Kyoung Tae Kim

Appl. Phys. Lett. 92, 251503 (2008); http://dx.doi.org/10.1063/1.2952496 (3 pages) | Cited 4 times

Online Publication Date: 27 June 2008

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Positive pulsed corona discharge has been applied for the oxidation of gaseous elemental mercury (Hg0) from a simulated flue gas. The oxidation of Hg0 to HgO and HgCl2 can significantly enhance the mercury removal from flue gas. At a gas condition of O2 (10%), H2O (3%), and N2 (balance), Hg0 oxidation efficiency of 84% was achieved at an input energy density of 45 J/l. The presence of NO, however, hinders Hg0 oxidation due to the preferential reaction of NO with O and O3. On the contrary, SO2 shows little effect on Hg0 oxidation due to its preferential reaction with OH. It has been also observed that the HCl in gas stream can be dissociated to Cl and Cl2 and can induce additional Hg0 oxidation to HgCl2.
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52.80.Hc Glow; corona
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