G. Kalinchenko
University of Michigan
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Publication
Featured researches published by G. Kalinchenko.
Optics Express | 2008
V. Yanovsky; V. Chvykov; G. Kalinchenko; P. Rousseau; T. Planchon; T. Matsuoka; Anatoly Maksimchuk; John A. Nees; Gilles Cheriaux; G. Mourou; Karl Krushelnick
We demonstrate the highest intensity - 300 TW laser by developing booster amplifying stage to the 50-TW-Ti:sapphire laser (HERCULES). To our knowledge this is the first multi-100TW-scale laser at 0.1 Hz repetition rate.
Optics Letters | 2006
V. Chvykov; P. Rousseau; S. Reed; G. Kalinchenko; V. Yanovsky
We demonstrate what we believe to be the highest-contrast (1011), multiterawatt, chirped-pulse amplification (CPA) Ti:sapphire laser by applying the modified cross-polarized-wave (XPW) generation method. This method produces a contrast improvement of 3 orders of magnitude using microjoule input energy. Microjoule energy can be achieved by direct amplification without the complications of a double CPA system. The 1011 contrast is sufficient for experiments on high-damage-threshold solid targets with focused intensities up to 1022 W/cm2.
Medical Physics | 2008
Stepan Bulanov; Andrei Brantov; Valery Yu. Bychenkov; V. Chvykov; G. Kalinchenko; T. Matsuoka; P. Rousseau; S. Reed; V. Yanovsky; K. Krushelnick; Dale W. Litzenberg; Anatoly Maksimchuk
Proton acceleration by high-intensity laser pulses from ultrathin foils for hadron therapy is discussed. With the improvement of the laser intensity contrast ratio to 10(-1) achieved on the Hercules laser at the University of Michigan, it became possible to attain laser-solid interactions at intensities up to 10(22) W/cm2 that allows an efficient regime of laser-driven ion acceleration from submicron foils. Particle-in-cell (PIC) computer simulations of proton acceleration in the directed Coulomb explosion regime from ultrathin double-layer (heavy ions/light ions) foils of different thicknesses were performed under the anticipated experimental conditions for the Hercules laser with pulse energies from 3 to 15 J, pulse duration of 30 fs at full width half maximum (FWHM), focused to a spot size of 0.8 microm (FWHM). In this regime heavy ions expand predominantly in the direction of laser pulse propagation enhancing the longitudinal charge separation electric field that accelerates light ions. The dependence of the maximum proton energy on the foil thickness has been found and the laser pulse characteristics have been matched with the thickness of the target to ensure the most efficient acceleration. Moreover, the proton spectrum demonstrates a peaked structure at high energies, which is required for radiation therapy. Two-dimensional PIC simulations show that a 150-500 TW laser pulse is able to accelerate protons up to 100-220 MeV energies.
Physics of Plasmas | 2010
Stepan Bulanov; Valery Yu. Bychenkov; V. Chvykov; G. Kalinchenko; Dale W. Litzenberg; T. Matsuoka; A. G. R. Thomas; L. Willingale; V. Yanovsky; K. Krushelnick; Anatoly Maksimchuk
The propagation of ultraintense laser pulses through matter is connected with the generation of strong moving magnetic fields in the propagation channel as well as the formation of a thin ion filament along the axis of the channel. Upon exiting the plasma the magnetic field displaces the electrons at the back of the target, generating a quasistatic electric field that accelerates and collimates ions from the filament. Two dimensional particle-in-cell simulations show that a 1 PW laser pulse tightly focused on a near-critical density target is able to accelerate protons up to an energy of 1.3 GeV. Scaling laws and optimal conditions for proton acceleration are established considering the energy depletion of the laser pulse.
Applied Optics | 2013
Vinay V. Alexander; Zhennan Shi; Mohammed N. Islam; Kevin Ke; G. Kalinchenko; Michael J. Freeman; Agustin I. Ifarraguerri; Joseph Meola; Anthony Absi; James Leonard; Jerome A. Zadnik; Anthony S. Szalkowski; Gregory J. Boer
Field trial results of a 5 W all-fiber broadband supercontinuum (SC) laser covering the short-wave infrared (SWIR) wavelength bands from ~1.55 to 2.35 μm are presented. The SC laser is kept on a 12 story tower at the Wright Patterson Air Force Base and propagated through the atmosphere to a target 1.6 km away. Beam quality of the SC laser after propagating through 1.6 km is studied using a SWIR camera and show a near diffraction limited beam with an M(2) value of <1.3. The SC laser is used as the illumination source to perform spectral reflectance measurements of various samples at 1.6 km, and the results are seen to be in good agreement with in-lab measurements using a conventional lamp source. Spectral stability measurements are performed after atmospheric propagation through 1.6 km and show a relative variability of ~4%-8% across the spectrum depending on the atmospheric turbulence effects. Spectral stability measurements are also performed in-lab and show a relative variability of <0.6% across the spectrum.
Physics of Plasmas | 2013
F. Dollar; C. Zulick; T. Matsuoka; C. McGuffey; S. S. Bulanov; V. Chvykov; J. Davis; G. Kalinchenko; G. M. Petrov; L. Willingale; V. Yanovsky; A. Maksimchuk; A. G. R. Thomas; K. Krushelnick
Ion acceleration from short pulse laser interactions at intensities of 2×1021Wcm−2 was studied experimentally under a wide variety of parameters, including laser contrast, incidence angle, and target thickness. Trends in maximum proton energy were observed, as well as evidence of improvement in the acceleration gradients by using dual plasma mirrors over traditional pulse cleaning techniques. Extremely high efficiency acceleration gradients were produced, accelerating both the contaminant layer and high charge state ions from the bulk of the target. Two dimensional particle-in-cell simulations enabled the study of the influence of scale length on submicron targets, where hydrodynamic expansion affects the rear surface as well as the front. Experimental evidence of larger electric fields for sharp density plasmas is observed in simulation results as well for such targets, where target ions are accelerated without the need for contaminant removal.
Applied Physics Letters | 2013
C. Zulick; F. Dollar; V. Chvykov; J. Davis; G. Kalinchenko; A. Maksimchuk; G. M. Petrov; A. Raymond; A. G. R. Thomas; L. Willingale; V. Yanovsky; K. Krushelnick
Experiments at the HERCULES laser facility have produced directional neutron beams with energies up to 16.8(±0.3) MeV using d12(d,n)23He,Li73(p,n)47Be,andLi37(d,n)48Be reactions. Efficient Li12(d,n)48Be reactions required the selective acceleration of deuterons through the introduction of a deuterated plastic or cryogenically frozen D2O layer on the surface of a thin film target. The measured neutron yield was ≤1.0 (±0.5)×107 neutrons/sr with a flux 6.2(±3.7) times higher in the forward direction than at 90°. This demonstrates that femtosecond lasers are capable of providing a time averaged neutron flux equivalent to commercial d12(d,n)23He generators with the advantage of a directional beam with picosecond bunch duration.
Applied Optics | 2008
V. Yanovsky; G. Kalinchenko; P. Rousseau; V. Chvykov; G. Mourou; Karl Krushelnick
A Nd:glass laser based on a novel design delivers up to 120 J energy pulses with a quasi-flat-top spatial profile at a 0.1 Hz repetition rate. The laser output is frequency-doubled with 50% efficiency and used to pump Ti:sapphire amplifiers. The developed design is perspective for use in the currently contemplated next step in ultra-high-intensity laser development.
Nuclear Fusion | 2010
T. Matsuoka; S. Reed; Christopher McGuffey; S. S. Bulanov; F. Dollar; L. Willingale; V. Chvykov; G. Kalinchenko; A. V. Brantov; V. Yu. Bychenkov; P. Rousseau; V. Yanovsky; Dale W. Litzenberg; K. Krushelnick; Anatoly Maksimchuk
The generation of energetic electron and proton beams was studied from the interaction of high intensity laser pulses with pre-drilled conical targets. These conical targets are laser machined onto flat targets using 7‐180 µJ pulses whose axis of propagation is identical to that of the main high intensity pulse. This method significantly relaxes requirements for alignment of conical targets in systematic experimental investigations and also reduces the cost of target fabrication. These experiments showed that conical targets increase the electron beam charge by up to 44 ± 18% compared with flat targets. We also found greater electron beam divergence for conical targets than for flat targets, which was due to escaping electrons from the surface of the cone wall into the surrounding solid target region. In addition, the experiments showed similar maximum proton energies for both targets since the larger electron beam divergence balances the increase in electron beam charge for conical targets. 2D particle in cell simulations were consistent with the experimental results. Simulations for conical target without preplasma showed higher energy gain for heavy ions due to ‘directed coulomb explosion’. This may be useful for medical applications or for ion beam fast ignition fusion.
Optics Letters | 2006
V. Chvykov; P. Rousseau; S. Reed; G. Kalinchenko; V. Yanovsky
We demonstrate what we believe to be the highest-contrast (10(11)), multiterawatt, chirped-pulse amplification (CPA) Ti:sapphire laser by applying the modified cross-polarized-wave (XPW) generation method. This method produces a contrast improvement of 3 orders of magnitude using microjoule input energy. Microjoule energy can be achieved by direct amplification without the complications of a double CPA system. The 10(11) contrast is sufficient for experiments on high-damage-threshold solid targets with focused intensities up to 10(22) W/cm(2).