8–12 Jul 2019
University of Milano-Bicocca UNIMIB
Europe/Rome timezone

Session

BPIF

8 Jul 2019, 16:30
Aula U6-06, Building U6 (University of Milano-Bicocca UNIMIB)

Aula U6-06, Building U6

University of Milano-Bicocca UNIMIB

Piazza dell’Ateneo Nuovo, 1 20126 Milan (Italy)

Conveners

BPIF

  • K. Lancaster

BPIF

  • L. Willingale (University of Michigan)

BPIF

  • S. Atzeni (Università di Roma "La Sapienza" and CNISM)

BPIF

  • L. Volpe (MIB)

BPIF

  • M. Vranic (GoLP/IPFN - Instituto Superior Tecnico)

BPIF

  • P. Muggli (Max-Planck-Institut für Physik)

Presentation materials

There are no materials yet.

  1. J.J. Rocca (EPS 2019)
    08/07/2019, 16:30
    BPIF

    See the full abstract here:
    http://ocs.ciemat.es/EPS2019ABS/pdf/I1.201.pdf

    The trapping of femtosecond laser pulses of relativistic intensity deep within ordered nanowire arrays can volumetrically heat dense matter into a new ultra-hot plasma regime [1]. Electron densities more than 100 times greater than the critical density with multi-keV temperatures are achieved using ultrashort laser...

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  2. M. Passoni (EPS 2019)
    08/07/2019, 17:00
    BPIF

    See the full abstract here:
    http://ocs.ciemat.es/EPS2019ABS/pdf/I1.202.pdf

    The investigation of superintense laser-driven ion sources and their potential applications offer unique opportunities of multisciplinary research [1]. Plasma physics can be combined with materials and nuclear science, radiation detection and advanced laser technology, leading to novel research challenges of great...

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  3. J.J. Santos (EPS 2019)
    08/07/2019, 17:30
    BPIF

    See the full abstract here:
    http://ocs.ciemat.es/EPS2019ABS/pdf/I1.203.pdf

    Generation of laser-driven quasi-static magnetic fields (B-fields), in the range of the kTesla, paves the ground for novel high energy-density physics (HEDP) investigations.
    I will review results and physical understanding in driving such strong B-fields. At LULI [Santos2015] and Gekko-XII [Law2016] laser facilities,...

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  4. H.T. Kim (EPS 2019)
    08/07/2019, 18:00
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/I1.204.pdf

    Laser wakefield acceleration (LWFA) can realize compact electron accelerators using significantly higher acceleration field than that of conventional rf accelerators. The progress of laser technologies reached PW peak power [1] and advanced the energy of laser electron accelerators to several GeV energy range [2,3]....

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  5. G. Cantono (EPS 2019)
    09/07/2019, 16:30
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/I2.201.pdf

    Experiments of laser-solid interaction at ultra-high contrast have recently demonstrated the possibility of exciting resonant propagating surface plasmons at relativistic intensities (> 10^18 W/cm^2) on solid grating targets [1]. Not only this encourages the development of a suitable theoretical description of plasmonic...

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  6. N. Lemos (EPS 2019)
    09/07/2019, 17:00
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/I2.202.pdf

    X-ray photon beams in the keV to MeV energy range are essential to study high energy density (HED) matter and to improve the understanding of inertial confinement fusion and astrophysical systems. HED experiments produce highly transient matter under extreme states of temperatures and pressures and it is essential to...

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  7. A. Andreev (EPS 2019)
    09/07/2019, 17:30
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O2.201.pdf

    Recently we have proposed an efficient scheme of generation of short dense electron bunches and atto-pulses during the interaction at large angles of incidence of a laser pulse with a limited foil target [1]. Later [2], the generation of high-intensity atto-pulses has been investigated also in a hollow cone-like target....

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  8. V. Annenkov (EPS 2019)
    09/07/2019, 17:45
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O2.202.pdf

    It was found recently [1] that counterpropagating plasma wakefields driven by a pair of femtosecond laser pulses with different transverse structures can produce powerful and narrowband EM emission near double plasma frequency. Such a nonlinear process can proceed in a homogeneous plasma, does not require the creation...

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  9. D. Kumar (EPS 2019)
    09/07/2019, 18:00
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O2.203.pdf

    At focused intensities above 10^18 W/cm^2, a laser pulse accelerates bunches of electrons into a solid target by the v x B component of the Lorentz force. These bunches are separated by half the laser period and hence emit visible light by coherent transition radiation (CTR) at twice the laser frequency (20) as they...

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  10. V. Smalyuk (EPS 2019)
    10/07/2019, 10:40
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/I3.201.pdf

    In Inertial Confinement Fusion (ICF), an indirectly driven implosion begins with an acceleration phase when the hohlraum x-rays ablate the shell surface and the capsule starts to converge. At this stage, outer-shell non-uniformities grow due to the acceleration-phase Richtmyer-Meshkov (RM) and Rayleigh≠Taylor (RT)...

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  11. S. Depierreux (EPS 2019)
    10/07/2019, 11:10
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/I3.202.pdf

    The direct and indirect drive schemes to ICF make use of a large number of laser beams arranged in a symmetric angular distribution. The preferential decay geometry of the three waves resonant couplings, mainly responsible for backscattered light in single beam experiments, may then be deeply modified in the region of...

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  12. K. Glize (EPS 2019)
    10/07/2019, 11:40
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O3.201.pdf

    Shock ignition is a promising route for laser fusion ignition; in principle high fusion energygain can be achieved with modest driver energies and hence capital investment.

    This talk will detail both simulations and ongoing collaborative experiments on the Omega, and NIF laser facilities. These are being performed both...

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  13. G. Ren (EPS 2019)
    10/07/2019, 11:55
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O3.202.pdf

    We design an octahedral spherical hohlraum with 6 laser entrance holes (LEHs) for the Rev. 6 Be ignition capsule [A. N. Simakov et al., Phys. Plasmas 21, 022701 (2014)]. With an Au spherical hohlraum of 4400 $\mu$m in radius and six LEHs of 1200 $\mu$m in radius, a laser pulse of 2.15 MJ energy and 630 TW power is...

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  14. P.A. Amendt (EPS 2019)
    10/07/2019, 12:10
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O3.203.pdf

    In indirect-drive inertial confinement fusion (ICF) a high-Z enclosure (or "hohlraum") surrounds a low-Z capsule containing DT fuel inside a low-Z spherical shell. Laser beams irradiate the interior of the hohlraum through a pair of laser entrance holes, in turn creating an x-ray radiation "bath" that compresses the...

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  15. R. Riquier (EPS 2019)
    10/07/2019, 12:25
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O3.204.pdf

    For the last couple of years, large efforts have been invested at CEA/DAM to develop the 3D radiationhydrodynamics code TROLL. Indeed, 2D radhydro codes are the main tool to design and analyze HED and ICF experiments. Yet, many of the first are intrinsically 3D, for example: few laser beams in directdrive or study...

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  16. A. Ruocco (EPS 2019)
    10/07/2019, 12:40
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O3.205.pdf

    The shock ignition (SI) approach to inertial confinement fusion promises ignition at a lower laser energy than conventional hotspot schemes. The target is initially driven at a low-implosion velocity, which reduces hydrodynamic instabilities, and then ignited by a high-intensity spikethat launches a strong shock into...

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  17. N. Iwata (EPS 2019)
    11/07/2019, 10:40
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/I4.201.pdf

    With the development of kJ, petawatt (PW) class lasers, laser pulses with relativistic intensities (>= 10^18 W/cm^2) and over-picosecond (ps) pulse durations are becoming available. In such a ps relativistic regime, the energy transfer enters in a new regime as indicated by the recent multi-ps PW laser experiments,...

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  18. P. Hilz (EPS 2019)
    11/07/2019, 11:10
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/I4.202.pdf

    Mass-Limited Targets (MLT) represent an interesting option for many applications, based on laser-plasma interactions. Various theoretical studies investigated MLT's extensively. Experimental verification of these schemes is extremely demanding, due to the technological challenges on targetry and requirements on the...

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  19. G. Lehmann (EPS 2019)
    11/07/2019, 11:40
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O4.201.pdf

    The manipulation of intense laser fields by solid-state devices is severely limited due to nonlinearities and damage threshold issues as the fluence of high-intensity laser pulses is more than five orders of magnitudes larger than what conventional materials can sustain. In recent years, novel concepts how structured...

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  20. G. Raj (EPS 2019)
    11/07/2019, 11:55
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O4.202.pdf

    During laser-solid target interactions, the onset of Weibel instability can generate super-strong magnetic field structures (up to several tens of MG) on the surface and within the bulk of the solid targets. Such magnetic fields can be used to understand several physical events in astrophysics such as blast wave shocks...

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  21. T. Frazer (EPS 2019)
    11/07/2019, 12:10
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O4.203.pdf

    A study of the influence of laser focal spot size on the acceleration of protons at intensities up to 5 x 10^21 Wcm^-2 is presented. Through the use of ellipsoidal, F/1 focusing plasma mirrors, focal spot sizes (~ 1.5 µm) on the order of the laser wavelength (1.054 µm) are achieved [1, 2]. Results are compared with...

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  22. L. Fedeli (EPS 2019)
    11/07/2019, 12:25
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O4.204.pdf

    Achieving a light source delivering intensities up to the Schwinger limit of 10^29W/cm^2 would allow exploring novel regimes of strong-field Quantum ElectroDynamics (QED) where vacuum would be ripped apart. A promising candidate to build such a light source would be to find a realistic implementation of the Curved...

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  23. G. Blaclard (EPS 2019)
    11/07/2019, 12:40
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O4.205.pdf

    The interaction of intense laser beams with plasmas created on solid targets involves a rich non-linear physics. Because such dense plasmas are reflective for laser light, the coupling with the incident beam occurs within a thin layer at the interface between plasma and vacuum. One of the main paradigms used to...

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  24. A. Huebl (EPS 2019)
    11/07/2019, 16:30
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/I4.203.pdf

    Since the very beginning, simulations have been an integral part of laser plasma research. With the advance of high-power lasers, non-linear effects on ultra-short time scales require extensive control in experimental setups, theoretical assumptions and simulation stability alike. For the latter, Particle-in-Cell...

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  25. A. Arefiev (EPS 2019)
    11/07/2019, 17:00
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/I4.204.pdf

    Newly constructed laser facilities such as ELI NP and ELI Beamlines are expected to deliver unprecedented laser intensities, making it possible to probe new regimes of light-matter interactions in laboratory conditions. One such regime is where a laser-irradiated solid material becomes relativistically transparent and...

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  26. L. Esnault (EPS 2019)
    11/07/2019, 17:30
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O4.206.pdf

    Despite being one of the most basic process of quantum electrodynamics (QED), and being responsible of the universe opacity to high energy photons [1], the electron-positron pair production by two photons collision (gamma-gamma -> e-e+, linear Breit-Wheeler [2] process, LBW) has never been observed directly in the...

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  27. R. Capdessus (EPS 2019)
    11/07/2019, 17:45
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O4.207.pdf

    When an ultra-intense laser pulse interacts with plasma, the accelerated electrons experience the back-radiation reaction due to the emission of electromagnetic radiation, and this has recently been experimentally evidenced [1]. The results suggest that both the quantum and classical nature of the back-radiation...

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  28. T. Silva (EPS 2019)
    11/07/2019, 18:00
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O4.208.pdf

    The interaction of intense electromagnetic waves with plasmas is a rich research topic. Magnetic fields play a crucial role in this context and there are several processes that can lead to the generation and amplification of these fields. Recent experiments, for instance, demonstrated the generation large-scale magnetic...

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  29. C. Xiao (EPS 2019)
    11/07/2019, 18:15
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O4.209.pdf

    Parametric instabilities in two- and three-dimensional configurations in inhomogeneous plasmas have been studied on a wide range of parameter space ranging from direct-drive scheme to shock ignition. These include the nonlinear evolutions of stimulated Raman scattering (SRS), stimulated Brillouin scattering (SBS), and...

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  30. P. Tomassini (EPS 2019)
    12/07/2019, 10:40
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/I5.201.pdf

    The production of high-quality electron bunches in Laser Wake Field Acceleration [1] relies on the possibility to inject ultra-low emittance bunches in the plasma wave. A new bunch injection scheme (Resonant Multi-Pulse Ionization, ReMPI) has been conceived and studied in which electrons extracted by ionization are...

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  31. A.E. Hussein (EPS 2019)
    12/07/2019, 11:10
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/I5.202.pdf

    Modern laser technology and the realization of high-intensity, short-pulse laser systems using Chirped-Pulse Amplification has led to the development of novel laser-based acceleration schemes. For high-intensity, picosecond duration pulses, where the pulse duration exceeds the plasma period, the laser pulse will expel...

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  32. C. Benedetti (EPS 2019)
    12/07/2019, 11:40
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O5.201.pdf

    We present modeling and experimental results concerning the guiding of relativistically intense laser pulses with peak power of 0.85 PW over a distance of 15 diffraction lengths. Laser guiding was achieved by increasing the focusing strength of a capillary discharge waveguide using laser inverse Bremsstrahlung heating....

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  33. E. Siminos (EPS 2019)
    12/07/2019, 11:55
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O5.202.pdf

    Intense, ultra-short electromagnetic pulses are enabling applications such as the control of motion in solids and the observation of reaction dynamics at the electronic level. While both high-intensity and carrier envelope phase (CEP) tunability are crucial, they are hard to obtain with current methods. Laser-plasma...

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  34. A. Savel'ev (EPS 2019)
    12/07/2019, 12:10
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O5.203.pdf

    We demonstrated efficient electron acceleration in the plasma channel with injection through the breaking of plasma waves generated by parametric instabilities. It was shown experimentally that in the case of optimal preplasma parameters femtosecond laser pulse with an intensity of 5x10^18 W/cm^2 and an energy of 50 mJ...

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  35. H. Peng (EPS 2019)
    12/07/2019, 12:25
    BPIF

    See the full abstract here http://ocs.ciemat.es/EPS2019ABS/pdf/O5.204.pdf

    The plasma devices can stand for much larger energy fluency than solid optical devices. Thus plasma devices become a hot topic recently, as the laser power is promoted to Petawatt order. Plasma grating is one of these appealing plasma devices. Plasma grating can act as laser polarizer and waveplate for both long,...

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