Miscellaneous publications

2019

G. Betancourt-Martinez, H. Akamatsu, D. Barret, M. Bautista, S. Bernitt, S. Bianchi, D. Bodewits, N. Brickhouse, G. V. Brown, E. Costantini, M. Coreno, J. R. C. Lopez-Urrutia, R. Cumbee, M. Eckart, G. Ferland, F. Fiore, M. Fogle, A. Foster, J. García, T. Gorczyca, V. Grinberg, N. Grosso, L. Gu, M. F. Gu, M. Guainazzi, N. Hell, J.-W. d. Herder, J. Kaastra, T. Kallman, J. Lee, M. Leutenegger, J. Marler, D. McCammon, S. Nakashima, F. Nicastro, F. Paerels, F. Pajot, E. Pointecouteau, D. Porquet, F. S. Porter, D. W. Savin, M. Sawada, C. Shah, A. Simionescu, M. d. Simone, C. Sosolik, P. Stancil, R. Steinbrügge, and H. Yamaguchi
Unlocking the Capabilities of Future High-Resolution X-ray Spectroscopy Missions Through Laboratory Astrophysics (March 2019)
File:https://arxiv.org/abs/1903.08213
R. Hollinger, V. Shumakova, A. Pugžlys, A. Baltuska, S. Khujanov, C. Spielmann, and D. Kartashov
High-order harmonic generation traces ultrafast coherent phonon dynamics in ZnO
XXI International Conference on Ultrafast Phenomena 2018 (UP 2018) ( 2019)
DOI
M. Zuerch, F. Tuitjea, T. Helk, J. Gautier, F. Tissandier, J. -P. Goddet, E. Oliva, A. Guggenmos, U. Kleineberg, H. Stiel, S. Sebban, and C. Spielmann
Lab-scale soft X-ray ptychography: advanced nanoscale imaging and beam diagnostics
X-Ray Lasers and Coherent X-Ray Sources: Development and Applications XIII ( 2019)
DOI
T. Sieber, H. D. Gersem, J. Golm, D. Haider, N. Marsic, W. Müller, H. Reeg, M. Schmelz, F. Schmidl, M. Schwickert, P. Seidel, T. Stöhlker, R. Stolz, J. Tan, G. Tranquille, V. Tympel, and V. Zakosarenko
Next Generation Cryogenic Current Comparator (CCC) for nA Intensity Measurement
10th International Particle Accelerator Conference ( 2019)
DOI
M. Zuerch, F. Tuitje, T. Helk, J. Gautier, F. Tissandier, J.-P. Goddet, A. Guggenmos, U. Kleineberg, S. Sebban, and C. Spielmann
Single shot XUV nanoimaging using an intense femtosecond soft X-ray laser
XXI International Conference on Ultrafast Phenomena 2018 (UP 2018) ( 2019)
DOI
D. Hoff, M. Krueger, L. Maisenbacher, A. Sayler, P. Hommelhoff, and G. Paulus
Tracing the phase of focused broadband laser pulses
, XXI International Conference on Ultrafast Phenomena 2018 (UP 2018)Volume13, Page 947 ( 2019)
DOI
M.C. Kaluza
Ultrafast Plasma Imaging
Springer Proc. Phys., 231 :165 ( 2019)
K. Huetten, M. Mittermair, S. Stock, R. Beerwerth, V. Shirvanyan, J. Riemensberger, A. Duensing, R. Heider, M. Wagner, A. Guggenmos, S. Fritzsche, N. Kabachnik, R. Kienberger, and B. Bernhardt
Ultrafast quantum control of ionization dynamics
XXI International Conference on Ultrafast Phenomena 2018 (UP 2018) ( 2019)
DOI

2017

J. Körner, J. Reiter, T. Lühder, J. Hein, V. Jambunathan, A. Lucianetti, T. Mocek, and M.C. Kaluza
Temperature dependent spectroscopic characterization of Tm:YAG crystals as potential laser medium for pulsed high energy laser amplifiers
SPIE Proceedings Volume 10238, High-Power, High-Energy, and High-Intensity Laser Technology III (May 2017)
DOI
J. Limpert
High Power Fiber Lasers
Optical Fiber Communication Conference 2017 (March 2017)
DOI
S. S. Bulanov, S. V. Bulanov, T. Zh. Esirkepov, M. Kando, S. Rykovanov, F. Pegoraro, C. B. Schroeder, E. Esarey, and W. P. Leemans
Strong field electrodynamics of a thin foil
, AIP Conference Proceedings 1812Volume1812, Page 090001 (March 2017)
DOI
V. Tympel, J. Golm, R. Neubert, P. Seidel, M. Schmelz, R. Stolz, V. Zakosarenko, F. Kurian, M. Schwickert, T. Sieber, and T. Stöhlker
The Next Generation of Cryogenic Current Comparators for Beam Monitoring (March 2017)
File:pdfhttp://accelconf.web.cern.ch/AccelConf/ibic2016/papers/proceed.pdf
M. Mueller, M. Kienel, A. Klenke, T. Gottschall, E. Shestaev, M. Plötner, J. Limpert, and A. Tünnermann
12 mJ pulse energy 8-channel divided-pulse ultrafast fiber-laser system
SPIE Proceedings Volume 10083, Fiber Lasers XIV: Technology and Systems (February 2017)
DOI
C. Stihler, C. Jauregui, H.-J. Otto, J. Limpert, and A. Tünnermann
Controlling mode instabilities at 628 W average output power in an Yb-doped rod-type fiber amplifier by active modulation of the pump power
SPIE Proceedings Volume 10083, Fiber Lasers XIV: Technology and Systems (February 2017)
DOI
H. Stark, M. Müller, M. Kienel, A. Klenke, J. Limpert, and A. Tünnermann
Divided-pulse amplification with fiber-coupled electro-optic modulators
SPIE Proceedings Volume 10083, Fiber Lasers XIV: Technology and Systems (February 2017)
DOI
C. Stihler, H.-J. Otto, C. Jauregui, J. Limpert, and A. Tünnermann
Experimental investigation of transverse mode instabilities in a double-pass Yb-doped rod-type fiber amplifier
SPIE Proceedings Volume 10083, Fiber Lasers XIV: Technology and Systems (February 2017)
DOI
M. Gebhardt, C. Gaida, F. Stutzki, S. Hädrich, C. Jauregui, J. Limpert, and A. Tünnermann
High-average power 4 GW pulses with sub-8 optical cycles from a Tm-doped fiber laser driven nonlinear pulse compression stage
SPIE Proceedings Volume 10083, Fiber Lasers XIV: Technology and Systems (February 2017)
DOI
K. Mecseki, H. T. Olgun, M. Windeler, M. Schulz, R. Riedel, F. Tavella, and M. J. Prandolini
Investigation of the critical parameters for CEP stabilized high power 1.5μm OPCPA
SPIE Proceedings Volume 10082, Solid State Lasers XXVI: Technology and Devices (February 2017)
DOI
C. Jauregui, M. Müller, M. Kienel, F. Emaury, C. J. Saraceno, J. Limpert, U. Keller, and A. Tünnermann
Optimizing the noise characteristics of high-power fiber laser systems
SPIE Proceedings Volume 10083, Fiber Lasers XIV: Technology and Systems (February 2017)
DOI
F. Stutzki, C. Gaida, M. Gebhardt, C. Jauregui, J. Limpert, A. Tünnermann, and I. Pupeza
Self-protecting nonlinear compression in a solid fiber for long-term stable ultrafast lasers at 2 µm wavelength
SPIE Proceedings Volume 10083, Fiber Lasers XIV: Technology and Systems (February 2017)
DOI
C. Jauregui, H.-J. Otto, C. Stihler, J. Limpert, and A. Tünnermann
The impact of core co-dopants on the mode instability threshold of high-power fiber laser systems
SPIE Proceedings Volume 10083, Fiber Lasers XIV: Technology and Systems (February 2017)
DOI
C. Gaida, M. Gebhardt, F. Stutzki, C. Jauregui, J. Limpert, and A. Tünnermann
Towards sub-100 fs multi-GW pulses directly emitted from a Thulium-doped fiber CPA system
SPIE Proceedings Volume 10083, Fiber Lasers XIV: Technology and Systems (February 2017)
DOI

2016

F. Karbstein
The quantum vacuum in electromagnetic fields: From the Heisenberg-Euler effective action to vacuum birefringence (December 2016)
File:pdfhttps://inspirehep.net/record/1501006/files/arXiv:1611.09883.pdf
D. Bernhardt, C. Brandau, Z. Harman, C. Kozhuharov, S. Böhm, F. Bosch, S. Fritzsche, J. Jacobi, S. Kieslich, H. Knopp, F. Nolden, W. Shi, Z. Stachura, M. Steck, T. Stöhlker, S. Schippers, and A. Müller
Erratum: Electron-ion collision spectroscopy: Lithium-like xenon ions [Phys. Rev. A 91, 012710 (2015)]
Phys. Rev. A, 94 :029903 (August 2016)
Abstract:
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2015

S. Schmidt, U. Lippmann, M. M. Guenther, and H. Gross
Diffraction effects in laser beam shaping systems
Proc. SPIE, 9626 :962610 (September 2015)
Abstract:
In modern laser-based ion acceleration systems, the field distribution of the focused laser beam at the position of the target strongly influences the overall characteristics of the resulting ion beam. To obtain an unidirectional and quasi mono-energetic ion beam, a flat-top field distribution of the focused laser beam is optimal. This can only be achieved, by using a beam-profiling system that reshapes the incident laser beam into an Airy-shaped field distribution in the far field. Here, we present an extensive design study of such a beam-profiling system based on two free-form mirrors. In order to realize the rings of zero intensity, corresponding to the roots of the Airy-function, strong curvature peaks on the first mirror are necessary. Additionally, the alternating phase in between these rings can only be achieved with grooves on the second mirror. These aspects actually raise the question, if the used purely geometric optical modeling approach is still valid. Therefore, our design study is entirely accompanied with wave-optical simulations to identify influences of diffraction within the beam profiling system. We find that especially the grooves on the second mirror are mandatory, not only to ensure the alternating phase, but also to realize the roots of zero intensity of the Airy-function. On the other hand, these grooves cause diffraction effects in the beam-profiling system that slightly degrade the at-top focal field. These influences are in the range of a few percent and cannot be further avoided.