Vladislav N. Ginzburg
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The organizations/institutes from the scholar's latest article
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Research Interests
Vladislav N. Ginzburg has a total of 16 co-authors. Here are the top co-authors by number of shared publications:
- Aleksandr V. Kotov
Institute of Applied Physics, Russian Academy of Sciences 2 , 46 Ulyanov st., Nizhny Novgorod 603951
2 shared publications - Alexander A. Soloviev
Russian Academy of Sciences
2 shared publications - Alexey A. Kuzmin
A.V. Gaponov-Grekhov Institute of Applied Physics of the Russian Academy of Sciences (IAP RAS), 46 Ulyanov St., Nizhny Novgorod 603950, Russia
2 shared publications - Andrey Shaykin
Gaponov-Grekhov Institute of Applied Physics of the Russian Academy of Sciences, N. Novgorod, Russia
2 shared publications - Anton A. Kochetkov
A.V. Gaponov-Grekhov Institute of Applied Physics of the Russian Academy of Sciences (IAP RAS), 46 Ulyanov St., Nizhny Novgorod 603950, Russia
2 shared publications - Efim Khazanov
Nonlinear Dynamics and Optics Division, Federal Research Center A.V. Gaponov-Grekhov Institute of Applied Physics of the Russian Academy of Sciences (IAP RAS), Nizhny Novgorod, Russia
2 shared publications
Latest Publications
- Open Access
Non-Ideal Hall MHD Rayleigh–Taylor Instability in Plasma Induced by Nanosecond and Intense Femtosecond Laser Pulses
A pioneering detailed comparative study of the dynamics of plasma flows generated by high-power nanosecond and high-intensity femtosecond laser pulses with similar fluences of up to J/cm2 is presented. The experiments were conducted on the petawatt laser facility PEARL using two types of high-power laser radiation: femtosecond pulses with energy exceeding 10 J and a duration less than 60 fs, and nanosecond pulses with energy exceeding 10 J and a duration on the order of 1 ns. In the experiments, high-velocity (>100 km/s) flows of «femtosecond» (created by femtosecond laser pulses) and «nanosecond» plasmas propagated in a vacuum across a uniform magnetic field with a strength over 14 T. A significant difference in the dynamics of «femtosecond» and «nanosecond» plasma flows was observed: (i) The «femtosecond» plasma initially propagated in a vacuum (no B-field) as a collimated flow, while the «nanosecond» flow diverged. (ii) The «nanosecond» plasma interacting with external magnetic field formed a quasi-spherical cavity with Rayleigh–Taylor instability flutes. In the case of «femtosecond» plasma, such flutes were not observed, and the flow was immediately redirected into a narrow plasma sheet (or «tongue») propagating across the magnetic field at an approximately constant velocity. (iii) Elongated «nanosecond» and «femtosecond» plasma slabs interacting with a transverse magnetic field broke up into Rayleigh–Taylor «tongues». (iv) The ends of these «tongues» in the femtosecond case twisted into vortex structures aligned with the ion motion in the external magnetic field, whereas the «tongues» in the nanosecond case were randomly oriented. It was suggested that the twisting of femtosecond «tongues» is related to Hall effects. The experimental results are complemented by and consistent with numerical 3D magnetohydrodynamic simulations. The potential applications of these findings for astrophysical objects, such as short bursts in active galactic nuclei, are discussed.Open AccessNon-Ideal Hall MHD Rayleigh–Taylor Instability in Plasma Induced by Nanosecond and Intense Femtosecond Laser Pulses
A pioneering detailed comparative study of the dynamics of plasma flows generated by high-power nanosecond and high-intensity femtosecond laser pulses with similar fluences of up to J/cm2 is presented. The experiments were conducted on the petawatt laser facility PEARL using two types of high-power laser radiation: femtosecond pulses with energy exceeding 10 J and a duration less than 60 fs, and nanosecond pulses with energy exceeding 10 J and a duration on the order of 1 ns. In the experiments, high-velocity (>100 km/s) flows of «femtosecond» (created by femtosecond laser pulses) and «nanosecond» plasmas propagated in a vacuum across a uniform magnetic field with a strength over 14 T. A significant difference in the dynamics of «femtosecond» and «nanosecond» plasma flows was observed: (i) The «femtosecond» plasma initially propagated in a vacuum (no B-field) as a collimated flow, while the «nanosecond» flow diverged. (ii) The «nanosecond» plasma interacting with external magnetic field formed a quasi-spherical cavity with Rayleigh–Taylor instability flutes. In the case of «femtosecond» plasma, such flutes were not observed, and the flow was immediately redirected into a narrow plasma sheet (or «tongue») propagating across the magnetic field at an approximately constant velocity. (iii) Elongated «nanosecond» and «femtosecond» plasma slabs interacting with a transverse magnetic field broke up into Rayleigh–Taylor «tongues». (iv) The ends of these «tongues» in the femtosecond case twisted into vortex structures aligned with the ion motion in the external magnetic field, whereas the «tongues» in the nanosecond case were randomly oriented. It was suggested that the twisting of femtosecond «tongues» is related to Hall effects. The experimental results are complemented by and consistent with numerical 3D magnetohydrodynamic simulations. The potential applications of these findings for astrophysical objects, such as short bursts in active galactic nuclei, are discussed. - Open Access
- 22 May 2025
- Published by MDPI AG in Preprints.org
Non-Ideal Hall MHD Rayleigh-Taylor Instability in Plasma Induced by Nanosecond and Intense Femtosecond Laser Pulses
A pioneer detailed comparative study of the dynamics of plasma flows generated by high-power nanosecond and high-intensity femtosecond laser pulses with similar fluences of up to 3 × 10^4 J/cm^2 is presented. The experiments were conducted on the petawatt laser facility PEARL using two types of high-power laser radiation: femtosecond pulses with energy exceeding 10 J, duration less than 60 fs, and nanosecond pulses with energy exceeding 10 J and duration on the order of 1 ns. In the experiments, high-velocity (>100 km/s) flows of femtosecond (created by femtosecond laser pulses) and nanosecond plasmas propagated in vacuum across a uniform magnetic field with a strength over 14 T. A significant difference in the dynamics of femtosecond and nanosecond plasma flows was observed: (i) The femtosecond plasma initially propagated in vacuum (no B-field) as a collimated flow, while the nanosecond flow diverged; (ii) The nanosecond plasma interacting with external magnetic field formed a quasi-spherical cavity with Rayleigh–Taylor instability flutes. In the case of femtosecond plasma, such flutes were not observed, and the flow was immediately redirected into a narrow plasma sheet (or tongue) propagating across the magnetic field at an approximately constant velocity; (iii) Elongated nanosecond and femtosecond plasma slabs interacting with a transverse magnetic field broke up into Rayleigh–Taylor tongues; (iv) The ends of these tongues in the femtosecond case twisted into vortex structures aligned with the ion motion in the external magnetic field, whereas the tongues in the nanosecond case were randomly oriented. It was suggested that the twisting of femtosecond tongues is related to Hall effects. The experimental results are complemented by and consistent with numerical 3D magnetohydrodynamic simulations. The potential applications of these findings for astrophysical objects, such as short bursts in active galactic nuclei, are discussed.
- 22 May 2025
- Published by MDPI AG in Preprints.org
Open AccessNon-Ideal Hall MHD Rayleigh-Taylor Instability in Plasma Induced by Nanosecond and Intense Femtosecond Laser Pulses
A pioneer detailed comparative study of the dynamics of plasma flows generated by high-power nanosecond and high-intensity femtosecond laser pulses with similar fluences of up to 3 × 10^4 J/cm^2 is presented. The experiments were conducted on the petawatt laser facility PEARL using two types of high-power laser radiation: femtosecond pulses with energy exceeding 10 J, duration less than 60 fs, and nanosecond pulses with energy exceeding 10 J and duration on the order of 1 ns. In the experiments, high-velocity (>100 km/s) flows of femtosecond (created by femtosecond laser pulses) and nanosecond plasmas propagated in vacuum across a uniform magnetic field with a strength over 14 T. A significant difference in the dynamics of femtosecond and nanosecond plasma flows was observed: (i) The femtosecond plasma initially propagated in vacuum (no B-field) as a collimated flow, while the nanosecond flow diverged; (ii) The nanosecond plasma interacting with external magnetic field formed a quasi-spherical cavity with Rayleigh–Taylor instability flutes. In the case of femtosecond plasma, such flutes were not observed, and the flow was immediately redirected into a narrow plasma sheet (or tongue) propagating across the magnetic field at an approximately constant velocity; (iii) Elongated nanosecond and femtosecond plasma slabs interacting with a transverse magnetic field broke up into Rayleigh–Taylor tongues; (iv) The ends of these tongues in the femtosecond case twisted into vortex structures aligned with the ion motion in the external magnetic field, whereas the tongues in the nanosecond case were randomly oriented. It was suggested that the twisting of femtosecond tongues is related to Hall effects. The experimental results are complemented by and consistent with numerical 3D magnetohydrodynamic simulations. The potential applications of these findings for astrophysical objects, such as short bursts in active galactic nuclei, are discussed.