Add to BibSonomyAbstract
Passive optical resonators are important tools for enhancing the sensitivity of spectroscopic measurements [1], and for enhancing the peak and average power of femtosecond laser pulses to the levels necessary for high-order harmonic generation (HHG), e.g. for the generation of XUV frequency combs [2]. The optical bandwidth and thus the pulse duration in such enhancement cavities (ECs) is typically limited by the spectral phase curvature inherent to the highly reflective multilayer mirrors.
© 2017 IEEE
PDF ArticleMore Like This
N. Lilienfein, M. Högner, C. Hofer, T. Saule, M. Trubetskov, V. Pervak, E. Fill, C. Riek, A. Leitenstorfer, J. Limpert, F. Krausz, and I. Pupeza
ef_10_4 European Quantum Electronics Conference (EQEC) 2019
S. Holzberger, N. Lilienfein, H. Carstens, T. Saule, F. Lücking, M. Trubetskov, V. Pervak, T. Eidam, J. Limpert, A. Tünnermann, E. Fill, F. Krausz, and I. Pupeza
CG_P_12 The European Conference on Lasers and Electro-Optics (CLEO/Europe) 2015
Tobias Saule, Maximilian Högner, Nikolai Lilienfein, Oliver deVries, Marco Plötner, Nicholas Karpowicz, Vladislav S. Yakovlev, Jens Limpert, Andreas Tünnermann, and Ioachim Pupeza
CD_P_18 The European Conference on Lasers and Electro-Optics (CLEO/Europe) 2017