Andy Steinmann
University of Stuttgart
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Publication
Featured researches published by Andy Steinmann.
Optics Letters | 2005
Alexander Killi; Andy Steinmann; Jochen Dörring; Uwe Morgner; Max Lederer; Daniel Kopf; Carsten Fallnich
We report generation of 1.35 microJ femtosecond laser pulses with a peak power of 3 MW at 1 MHz repetition rate from a diode-pumped Yb:KY(WO4)2 laser oscillator with cavity dumping. By extracavity compression with a large-mode-area fiber and a prism sequence, we generate ultrashort pulses with a duration of 21 fs and a peak power of 13 MW.
Optics Letters | 2012
Robin Hegenbarth; Andy Steinmann; Sergey Yu. Sarkisov; Harald Giessen
We demonstrate the generation of mid-infrared radiation using a femtosecond dual-signal-wavelength optical parametric oscillator and difference frequency generation in an extracavity gallium selenide or silver gallium diselenide crystal. This system generates up to 4.3 mW of average mid-infrared power. Its spectra can be tuned to between 10.5 μm and 16.5 μm wavelength (952 cm(-1)-606 cm(-1)) with more than 50 cm(-1) spectral bandwidth. We demonstrate that the power and spectra of this system are temporally very stable.
Optics Express | 2007
Guido Palmer; Moritz Emons; Martin Siegel; Andy Steinmann; Marcel Schultze; Max Lederer; Uwe Morgner
We demonstrate, what is to our knowledge the first passively mode-locked Ytterbium based solid state high energy laser oscillator operated in the positive dispersion regime. Compared to solitary mode-locking the pulse energy can be increased with even broader spectral bandwidth. With high speed cavity dumping the laser generates 2 µJ-pulses at a 1 MHz repetition rate. The chirped output pulses are compressible down to 420 fs.
Optics Express | 2009
Matthias Pospiech; Moritz Emons; Andy Steinmann; Guido Palmer; Roberto Osellame; Nicola Bellini; Giulio Cerullo; Uwe Morgner
We report on a novel method to create waveguide coupler devices in fused silica by combining the technique of beam shaping with femtosecond laser writing. The method is based on a programmable phase modulator and a dynamic variation of the phase-pattern during the writing process. The major advantage is the possibility to create complex devices in a single sweep by simultaneously writing two or more waveguides with changing separation. The guiding properties and the coupling behavior between the waveguides are investigated.
Optics Letters | 2007
Marco Marangoni; Roberto Osellame; Roberta Ramponi; Giulio Cerullo; Andy Steinmann; Uwe Morgner
We demonstrate a high-average-power optical parametric amplifier directly pumped by a cavity-dumped Yb:KYW mode-locked laser oscillator at 1 MHz repetition rate. The two-stage system uses periodically poled lithium niobate crystals both for optical parametric generation and for power amplification. We obtain average powers as high as 190 mW with 220 fs average pulse widths and wavelength tunability in the 1.3-1.6 microm (signal) and 3.1-4.6 microm (idler) range.
Optics Express | 2006
Andy Steinmann; Alexander Killi; Guido Palmer; Thomas Binhammer; Uwe Morgner
We demonstrate the generation of 10-fs-pulses from a noncollinear optical parametric amplifier (NOPA). The NOPA is driven by microjoule pulses from a directly diode pumped Yb:KYW oscillator with cavity-dumping.
Optics Letters | 2007
Guido Palmer; Martin Siegel; Andy Steinmann; Uwe Morgner
We demonstrate, for the first time to our knowledge, a passively mode-locked femtosecond thin-disk oscillator with cavity dumping. A beta-barium-borate-based pockels cell imposes cavity dumping at a repetition rate of 1 MHz. The laser generates pulse energies up to 3 microJ with a pulse duration of 680 fs in a diffraction-limited beam.
Optics Letters | 2006
Alexander Killi; Andy Steinmann; Guido Palmer; Uwe Morgner; Hartmut Bartelt; Jens Kobelke
We demonstrate, for the first time to our knowledge, an optical parametric amplifier directly pumped by a femtosecond oscillator. Wavelength-tunable pulses in the ranges 0.65-0.85 microm (signal) and 1.4-2.5 microm (idler) are generated at a repetition frequency of 1 MHz. For pumping the beta-barium borate crystal we use a microjoule Yb:KY(WO4)2 femtosecond oscillator with cavity dumping. Pulses with 30 nJ of energy and a duration of 16 fs are achieved from a supercontinuum seed generated in a sapphire plate.
Optics Letters | 2015
S. Chaitanya Kumar; Joachim Krauth; Andy Steinmann; Kevin T. Zawilski; Peter G. Schunemann; Harald Giessen; Majid Ebrahim-Zadeh
We report a femtosecond optical parametric oscillator (OPO) for the mid-infrared (mid-IR), generating a record average power of 110 mW at 7 μm. The OPO, based on CdSiP(2) (CSP) as the nonlinear crystal, provides idler wavelength tuning across 6540-7186 nm with spectral bandwidths >400 nm at -10 dB level over the entire range, and a maximum bandwidth of 478 nm at 6.9 μm. To the best of our knowledge, this is the highest average power generated from a femtosecond OPO in the deep mid-IR. The OPO also provides near-IR signal wavelengths tunable across 1204-1212 nm with a usable power of 450 mW in 418-fs pulses at 1207 nm. The simultaneously measured signal and idler power exhibit a passive stability better than 1.6% rms and 3% rms, respectively. A mid-IR idler spectral stability with a standard deviation of the frequency fluctuations better than 40 MHz over 15 min, limited by the measurement resolution, is realized. Using the mid-IR idler from the CSP OPO, we perform Fourier-transform spectroscopy to detect liquid phase organic solvent, toluene (C(7)H(8)), in the molecular fingerprint region.
Optics Express | 2010
Marcel Schultze; Thomas Binhammer; Andy Steinmann; Guido Palmer; Moritz Emons; Uwe Morgner
We present an OPCPA system delivering 8.8 fs (3.3 optical cycles) pulses with 1.3 microJ of energy at 143 kHz repetition rate. Pump and seed for the parametric amplification are simultaneously generated by a broadband Ti:sapphire oscillator. The spectral components beyond 1000 nm are separated and amplified in an Yb:YAG thin-disk regenerative amplifier. The pulses are characterized using autocorrelation and SPIDER apparatus. With a pulse peak power of nearly 130 MW, the system is well-suited for future table top strong field experiments.