Tibor Gilinger
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Tibor Gilinger has a total of 20 co-authors. Here are the top co-authors by number of shared publications:
- Karoly Osvay
National Laser-Initiated Transmutation Laboratory, University of Szeged, Szeged, Hungary
4 shared publications - Attila Pál Kovács
University of Szeged
3 shared publications - Miklós Füle
University of Szeged
3 shared publications - Peter Gaal
Department of Optics and Quantum Electronics, University of Szeged, Dóm tér 9, H-6720 Szeged, Hungary
3 shared publications - Adam Kovacs
National Laboratory for Cooperative Technologies, University of Szeged, 6720 Szeged, Hungary
2 shared publications - Balint Nagyilles
National Laser-Initiated Transmutation Laboratory, University of Szeged, 6720 Szeged, Hungary
2 shared publications
Latest Publications
- Open Access
- 25 August 2025
- Published by Springer Nature in Communications Physics
- Vol. 8 (1) , 1-12
Distinguished role of the laser pulse temporal structure on deuteron acceleration
- 25 August 2025
- Published by Springer Nature in Communications Physics
- Vol. 8 (1) , 1-12
Open AccessDistinguished role of the laser pulse temporal structure on deuteron acceleration
- Open Access
- 18 November 2024
- Published by MDPI AG in Applied Sciences
- Vol. 14 (22) , 10649
A Versatile 100 Hz Laser System with Few-Cycle and TeraWatt Pulses for Applications
We developed a versatile 100 Hz laser system based on negatively and positively chirped pulse amplification. The few-cycle output provides pulses with 7.1 fs and 0.25 mJ, while the power output supports 26 fs pulses with 50 mJ. The energy as well as the pulse duration stability of the system are below 1%, while the pointing stability is within 25% of the diffraction-limited spot size. We also show applications in high repetition rate target development and preparation for a laser-generated X-ray source for industrial CT imaging.
- 18 November 2024
- Published by MDPI AG in Applied Sciences
- Vol. 14 (22) , 10649
Open AccessA Versatile 100 Hz Laser System with Few-Cycle and TeraWatt Pulses for Applications
We developed a versatile 100 Hz laser system based on negatively and positively chirped pulse amplification. The few-cycle output provides pulses with 7.1 fs and 0.25 mJ, while the power output supports 26 fs pulses with 50 mJ. The energy as well as the pulse duration stability of the system are below 1%, while the pointing stability is within 25% of the diffraction-limited spot size. We also show applications in high repetition rate target development and preparation for a laser-generated X-ray source for industrial CT imaging.
- Open Access
- 3 October 2024
- Published by MDPI AG in Preprints.org
A Versatile 100 Hz Laser System with Few-Cycle and TW Pulses for Applications
We developed a versatile 100 Hz laser system based on negatively and positively chirped pulse amplification. The few-cycle output provides pulses with 7.1 fs and 0.25 mJ, while the power output supports 26 fs pulses with 50 mJ. The energy as well as the pulse duration stability of the system is below 1%, while the pointing stability is within 25% of the diffraction limited spot size. We also show applications in high repetition rate target development and preparation for a laser-generated X-ray source for industrial CT imaging.
- 3 October 2024
- Published by MDPI AG in Preprints.org
Open AccessA Versatile 100 Hz Laser System with Few-Cycle and TW Pulses for Applications
We developed a versatile 100 Hz laser system based on negatively and positively chirped pulse amplification. The few-cycle output provides pulses with 7.1 fs and 0.25 mJ, while the power output supports 26 fs pulses with 50 mJ. The energy as well as the pulse duration stability of the system is below 1%, while the pointing stability is within 25% of the diffraction limited spot size. We also show applications in high repetition rate target development and preparation for a laser-generated X-ray source for industrial CT imaging.
- Open Access
- 1 April 2024
- Published by Cambridge University Press (CUP) in High Power Laser Science and Engineering
- Vol. 12, 1-24
Development of an ultrathin liquid sheet target for laser ion acceleration at high repetition rates in the kilohertz range
A colliding microjet liquid sheet target system was developed and tested for pairs of round nozzles of 10, 11 and 18 μm in diameter. The sheet’s position stability was found to be better than a few micrometers. Upon interaction with 50 mJ laser pulses, the 18 μm jet has a resonance amplitude of 16 μm at a repetition rate of 33 Hz, while towards 100 Hz it converges to 10 μm for all nozzles. A white-light interferometric system was developed to measure the liquid sheet thickness in the target chamber both in air and in vacuum, with a measurement range of 182 nm–1 μm and an accuracy of ±3%. The overall shape and 3D shape of the sheet follow the Hasson–Peck model in air. In vacuum versus air, the sheet gradually loses 10% of its thickness, so the thinnest sheet achieved was below 200 nm at a vacuum level of 10–4 mbar, and remained stable for several hours of operation.
- 1 April 2024
- Published by Cambridge University Press (CUP) in High Power Laser Science and Engineering
- Vol. 12, 1-24
Open AccessDevelopment of an ultrathin liquid sheet target for laser ion acceleration at high repetition rates in the kilohertz range
A colliding microjet liquid sheet target system was developed and tested for pairs of round nozzles of 10, 11 and 18 μm in diameter. The sheet’s position stability was found to be better than a few micrometers. Upon interaction with 50 mJ laser pulses, the 18 μm jet has a resonance amplitude of 16 μm at a repetition rate of 33 Hz, while towards 100 Hz it converges to 10 μm for all nozzles. A white-light interferometric system was developed to measure the liquid sheet thickness in the target chamber both in air and in vacuum, with a measurement range of 182 nm–1 μm and an accuracy of ±3%. The overall shape and 3D shape of the sheet follow the Hasson–Peck model in air. In vacuum versus air, the sheet gradually loses 10% of its thickness, so the thinnest sheet achieved was below 200 nm at a vacuum level of 10–4 mbar, and remained stable for several hours of operation.