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Dive into the research topics where S. S. Bulanov is active.

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Featured researches published by S. S. Bulanov.


Physical Review Letters | 2015

Active Plasma Lensing for Relativistic Laser-Plasma-Accelerated Electron Beams

J. van Tilborg; S. Steinke; C. G. R. Geddes; N. H. Matlis; Brian Shaw; A. J. Gonsalves; Julius Huijts; K. Nakamura; J. Daniels; C. B. Schroeder; C. Benedetti; E. Esarey; S. S. Bulanov; N. A. Bobrova; Pavel V. Sasorov; W. P. Leemans

Compact, tunable, radially symmetric focusing of electrons is critical to laser-plasma accelerator (LPA) applications. Experiments are presented demonstrating the use of a discharge-capillary active plasma lens to focus 100-MeV-level LPA beams. The lens can provide tunable field gradients in excess of 3000 T/m, enabling cm-scale focal lengths for GeV-level beam energies and allowing LPA-based electron beams and light sources to maintain their compact footprint. For a range of lens strengths, excellent agreement with simulation was obtained.


Physics of Plasmas | 2015

Generation and pointing stabilization of multi-GeV electron beams from a laser plasma accelerator driven in a pre-formed plasma waveguidea)

A. J. Gonsalves; K. Nakamura; J. Daniels; H.-S. Mao; C. Benedetti; C. B. Schroeder; Cs. Toth; J. van Tilborg; D. E. Mittelberger; S. S. Bulanov; J.-L. Vay; C. G. R. Geddes; E. Esarey; W. P. Leemans

Laser pulses with peak power 0.3u2009PW were used to generate electron beams with energy >4u2009GeV within a 9u2009cm-long capillary discharge waveguide operated with a plasma density of ≈7×1017u2009cm−3. Simulations showed that the super-Gaussian near-field laser profile that is typical of high-power femtosecond laser systems reduces the efficacy of guiding in parabolic plasma channels compared with the Gaussian laser pulses that are typically simulated. In the experiments, this was mitigated by increasing the plasma density and hence the contribution of self-guiding. This allowed for the generation of multi-GeV electron beams, but these had angular fluctuation ≳2u2009mrad rms. Mitigation of capillary damage and more accurate alignment allowed for stable beams to be produced with energy 2.7±0.1u2009GeV. The pointing fluctuation was 0.6u2009mrad rms, which was less than the beam divergence of ≲1u2009mrad full-width-half-maximum.


Physics of Plasmas | 2012

Optimized laser pulse profile for efficient radiation pressure acceleration of ions

S. S. Bulanov; C. B. Schroeder; E. Esarey; W. P. Leemans

The radiation pressure acceleration regime of laser ion acceleration requires high intensity laser pulses to function efficiently. Moreover, the foil should be opaque for incident radiation during the interaction to ensure maximum momentum transfer from the pulse to the foil, which requires proper matching of the target to the laser pulse. However, in the ultrarelativistic regime, this leads to large acceleration distances, over which the high laser intensity for a Gaussian laser pulse must be maintained. It is shown that proper tailoring of the laser pulse profile can significantly reduce the acceleration distance, leading to a compact laser ion accelerator, requiring less energy to operate.


Physics of Plasmas | 2013

Laser-heater assisted plasma channel formation in capillary discharge waveguides

N. A. Bobrova; Pavel V. Sasorov; C. Benedetti; S. S. Bulanov; C. G. R. Geddes; C. B. Schroeder; E. Esarey; W. P. Leemans

A method of creating plasma channels with controllable depth and transverse profile for the guiding of short, high power laser pulses for efficient electron acceleration is proposed. The plasma channel produced by the hydrogen-filled capillary discharge waveguide is modified by a ns-scale laser pulse, which heats the electrons near the capillary axis. This interaction creates a deeper plasma channel within the capillary discharge that evolves on a ns-time scale, allowing laser beams with smaller spot sizes than would otherwise be possible in the unmodified capillary discharge.


Physics of Plasmas | 2017

Plasma equilibrium inside various cross-section capillary discharges

G. A. Bagdasarov; Pavel V. Sasorov; A. S. Boldarev; O. G. Olkhovskaya; V. A. Gasilov; A. J. Gonsalves; S. K. Barber; S. S. Bulanov; C. B. Schroeder; J. van Tilborg; E. Esarey; W. P. Leemans; T. Levato; D. Margarone; G. Korn; S. V. Bulanov

Plasma properties inside a hydrogen-filled capillary discharge waveguide were modeled with dissipative magnetohydrodynamic simulations to enable analysis of capillaries of circular and square cross-sections implying that square capillaries can be used to guide circularly symmetric laser beams. When the quasistationary stage of the discharge is reached, the plasma and temperature in the vicinity of the capillary axis have almost the same profile for both the circular and square capillaries. The effect of cross-section on the electron beam focusing properties was studied using the simulation-derived magnetic field map. Particle tracking simulations showed only slight effects on the electron beam symmetry in the horizontal and diagonal directions for square capillary.


Physics of Plasmas | 2017

Laser beam coupling with capillary discharge plasma for laser wakefield acceleration applications

G. A. Bagdasarov; Pavel V. Sasorov; V. A. Gasilov; A. S. Boldarev; O. G. Olkhovskaya; C. Benedetti; S. S. Bulanov; A. J. Gonsalves; H.-S. Mao; C. B. Schroeder; J. van Tilborg; E. Esarey; W. P. Leemans; T. Levato; D. Margarone; G. Korn

One of the most robust methods, demonstrated to date, of accelerating electron beams by laser-plasma sources is the utilization of plasma channels generated by the capillary discharges. Although the spatial structure of the installation is simple in principle, there may be some important effects caused by the open ends of the capillary, by the supplying channels etc., which require a detailed 3D modeling of the processes. In the present work, such simulations are performed using the code MARPLE. First, the process of capillary filling with cold hydrogen before the discharge is fired, through the side supply channels is simulated. Second, the simulation of the capillary discharge is performed with the goal to obtain a time-dependent spatial distribution of the electron density near the open ends of the capillary as well as inside the capillary. Finally, to evaluate the effectiveness of the beam coupling with the channeling plasma wave guide and of the electron acceleration, modeling of the laser-plasma int...


Physics of Plasmas | 2017

On production and asymmetric focusing of flat electron beams using rectangular capillary discharge plasmas

G. A. Bagdasarov; N. A. Bobrova; A. S. Boldarev; O. G. Olkhovskaya; Pavel V. Sasorov; V. A. Gasilov; S. K. Barber; S. S. Bulanov; A. J. Gonsalves; C. B. Schroeder; J. van Tilborg; E. Esarey; W. P. Leemans; T. Levato; D. Margarone; G. Korn; M. Kando; S. V. Bulanov

A method for the asymmetric focusing of electron bunches, based on the active plasma lensing technique is proposed. This method takes advantage of the strong inhomogeneous magnetic field generated inside the capillary discharge plasma to focus the ultrarelativistic electrons. The plasma and magnetic field parameters inside the capillary discharge are described theoretically and modeled with dissipative magnetohydrodynamic computer simulations enabling analysis of the capillaries of rectangle cross-sections. Large aspect ratio rectangular capillaries might be used to transport electron beams with high emittance asymmetries, as well as assist in forming spatially flat electron bunches for final focusing before the interaction point.


IEEE Computer Graphics and Applications | 2016

WarpIV: In Situ Visualization and Analysis of Ion Accelerator Simulations

Oliver Rübel; Burlen Loring; Jean Luc Vay; David P. Grote; R. Lehe; S. S. Bulanov; Henri Vincenti; E. Wes Bethel

The generation of short pulses of ion beams through the interaction of an intense laser with a plasma sheath offers the possibility of compact and cheaper ion sources for many applications--from fast ignition and radiography of dense targets to hadron therapy and injection into conventional accelerators. To enable the efficient analysis of large-scale, high-fidelity particle accelerator simulations using the Warp simulation suite, the authors introduce the Warp In situ Visualization Toolkit (WarpIV). WarpIV integrates state-of-the-art in situ visualization and analysis using VisIt with Warp, supports management and control of complex in situ visualization and analysis workflows, and implements integrated analytics to facilitate query- and feature-based data analytics and efficient large-scale data analysis. WarpIV enables for the first time distributed parallel, in situ visualization of the full simulation data using high-performance compute resources as the data is being generated by Warp. The authors describe the application of WarpIV to study and compare large 2D and 3D ion accelerator simulations, demonstrating significant differences in the acceleration process in 2D and 3D simulations. WarpIV is available to the public via https://bitbucket.org/berkeleylab/warpiv. The Warp In situ Visualization Toolkit (WarpIV) supports large-scale, parallel, in situ visualization and analysis and facilitates query- and feature-based analytics, enabling for the first time high-performance analysis of large-scale, high-fidelity particle accelerator simulations while the data is being generated by the Warp simulation suite. This supplemental material https://extras.computer.org/extra/mcg2016030022s1.pdf provides more details regarding the memory profiling and optimization and the Yee grid recentering optimization results discussed in the main article.


Proceedings of SPIE | 2015

Maximum attainable ion energy in the radiation pressure acceleration regime

S. S. Bulanov; E. Esarey; C. B. Schroeder; S. V. Bulanov; Timur Zh. Esirkepov; M. Kando; Francesco Pegoraro; W. P. Leemans

The laser group velocity plays a crucial role in laser driven acceleration of electrons and ions. In particular, a highly efficient mechanism of laser driven ion acceleration, Radiation Pressure Acceleration, has a fundamental limit on the maximum attainable ion energy, which is determined by the group velocity of the laser. However there is another limiting factor that may shed the group velocity effects. It is due to the transverse expansion of the target, which happens in the course of a tightly focused laser pulse interaction with a thin foil. Transversely expanding targets become increasingly transparent for radiation thus terminating the acceleration. Utilization of an external guiding structure for the accelerating laser pulse may provide a way of compensating for the group velocity and transverse expansion effects.


Proceedings of SPIE | 2015

Ultra-low emittance beam generation using two-color ionization injection in laser-plasma accelerators

C. B. Schroeder; C. Benedetti; S. S. Bulanov; Min Chen; E. Esarey; Cameron Geddes; Jean-Luc Vay; Lule Yu; W. P. Leemans

Ultra-low emittance (tens of nm) beams can be generated in a plasma accelerator using ionization injection of electrons into a wakefield. An all-optical method of beam generation uses two laser pulses of different colors. A long-wavelength drive laser pulse (with a large ponderomotive force and small peak electric field) is used to excite a large wakefield without fully ionizing a gas, and a short-wavelength injection laser pulse (with a small ponderomotive force and large peak electric field), co-propagating and delayed with respect to the pump laser, to ionize a fraction of the remaining bound electrons at a trapped wake phase, generating an electron beam that is accelerated in the wake. The trapping condition, the ionized electron distribution, and the trapped bunch dynamics are discussed. Expressions for the beam transverse emittance, parallel and orthogonal to the ionization laser polarization, are derived. An example is presented using a 10-µm CO2 laser to drive the wake and a frequency-doubled Ti:Al2O3 laser for ionization injection.

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C. B. Schroeder

Lawrence Berkeley National Laboratory

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E. Esarey

Lawrence Berkeley National Laboratory

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W. P. Leemans

Lawrence Berkeley National Laboratory

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A. J. Gonsalves

Lawrence Berkeley National Laboratory

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C. Benedetti

Lawrence Berkeley National Laboratory

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Pavel V. Sasorov

Keldysh Institute of Applied Mathematics

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H.-S. Mao

Lawrence Berkeley National Laboratory

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J. Daniels

Lawrence Berkeley National Laboratory

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Cameron Geddes

Lawrence Berkeley National Laboratory

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J. van Tilborg

Lawrence Berkeley National Laboratory

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