Abstract:Intense few-cycle laser pulses as short as 5.1 fs are generated though self-filamentation in a noble gas atmosphere. We study the dependence of the laser pulse fidelity on the driving pulse profile and chirp as well as on the gas parameters, quantify their pointing stability and spatial quality.
“…However, the pulse output energy is limited by the critical power that is relatively low in high gas pressure required with this approach. Similar limit exist with filament based post compression [4].…”
Abstract. By using optical-field-ionization of helium we postcompress 50 fs pulses to 8 fs with a pulse energy of 8,7 mJ. Hence few cycle pulses were obtained with TW peak power and a good shot-to-shot stability.
“…However, the pulse output energy is limited by the critical power that is relatively low in high gas pressure required with this approach. Similar limit exist with filament based post compression [4].…”
Abstract. By using optical-field-ionization of helium we postcompress 50 fs pulses to 8 fs with a pulse energy of 8,7 mJ. Hence few cycle pulses were obtained with TW peak power and a good shot-to-shot stability.
“…The numerical and analytical solutions of AE (1) and DE (2) are equal to the solutions of the equations AE (8) and DE (9) in Galilean coordinates with only one difference: in Laboratory frame the solutions translate in z-direction , while in Galilean frame the solutions stay in the centrum of the coordinate system. The basic theoretical studies governed laser pulse propagation have been performed in so called "local time" coordinates z = z; τ = t − z/v gr .…”
Section: Linear Regime Of Narrow Band and Broad Band Optical Pulsesmentioning
“…III A and III B, the second scheme was adopted and 1.3-mJ pulses were sent through two filament cells filled with argon for spectral broadening. 30,31 The residual group-delay dispersion was compensated with broadband chirped mirrors. Pulses with energies of ∼350 μJ and a time duration down to ∼5.5 fs were achieved.…”
Section: A Coupling and Generation Chambersmentioning
We present our attoline which is a versatile attosecond beamline at the Ultrafast Laser Physics Group at ETH Zurich for attosecond spectroscopy in a variety of targets. High-harmonic generation (HHG) in noble gases with an infrared (IR) driving field is employed to generate pulses in the extreme ultraviolet (XUV) spectral regime for XUV-IR cross-correlation measurements. The IR pulse driving the HHG and the pulse involved in the measurements are used in a non-collinear set-up that gives independent access to the different beams. Single attosecond pulses are generated with the polarization gating technique and temporally characterized with attosecond streaking. This attoline contains two target chambers that can be operated simultaneously. A toroidal mirror relay-images the focus from the first chamber into the second one. In the first interaction region a dedicated double-target allows for a simple change between photoelectron/photoion measurements with a time-of-flight spectrometer and transient absorption experiments. Any end station can occupy the second interaction chamber. A surface analysis chamber containing a hemispherical electron analyzer was employed to demonstrate successful operation. Simultaneous RABBITT measurements in two argon jets were recorded for this purpose.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.