English (United Kingdom)

https://curated-unify.zendy.io/wp-json/zendy-region/v1/featured_content/oa?rat=en

https://curated-unify.zendy.io/wp-json/zendy-region/v1/highlighted_journal/

Global: Zendy Plus annual

Presents the access of premium content as premium feature

Premium Content

Presents the keyphrase highlighting as premium feature

Keyphrase Highlighting

Presents the summarisation as premium feature

Summarisation

Insights

Presents the pdf analysis as premium feature

PDF Analysis

Presents the zaia usage as premium feature

ZAIA

Global: Zendy Plus monthly

Global: Zendy Tools annual

Global: Zendy Tools monthly

Global: Zendy Free Plan

Optical Parametric Chirped-Pulse Amplification (OPCPA) (Dubietis et al., 1992, 2006) has attracted a lot of attention as a promising route toward intensity scaling of few-cycle laser pulses. Intense carrier-envelope phase (CEP)-stable few-cycle laser pulses have numerous intriguing applications in attosecond and high-field science (for a recent review, see Krausz & Ivanov, 2009) including the production of attosecond XUV/soft-X-ray pulses by high-harmonic generation (HHG) (Hentschel et al., 2001; Kienberger et al., 2004; Sansone et al., 2006), tomographic imaging of molecular orbitals (Itatani et al., 2004), and laser-induced electron diffraction (Meckel et al., 2008). A major challenge for using HHG in studies of time-resolved tomography of molecular dissociative states is the low ionization potential

Toward TW-Peak-Power Single-Cycle IR Fields for Attosecond Physics and High-Field Science