G. Kalintchenko
University of Michigan
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Featured researches published by G. Kalintchenko.
Applied Physics Letters | 2011
S. Kneip; C. McGuffey; F. Dollar; M. S. Bloom; V. Chvykov; G. Kalintchenko; K. Krushelnick; Anatoly Maksimchuk; S. P. D. Mangles; T. Matsuoka; Z. Najmudin; C. A. J. Palmer; J. Schreiber; W. Schumaker; A. G. R. Thomas; V. Yanovsky
We show that x-rays from a recently demonstrated table top source of bright, ultrafast, coherent synchrotron radiation [Kneip et al., Nat. Phys. 6, 980 (2010)] can be applied to phase contrast imaging of biological specimens. Our scheme is based on focusing a high power short pulse laser in a tenuous gas jet, setting up a plasma wakefield accelerator that accelerates and wiggles electrons analogously to a conventional synchrotron, but on the centimeter rather than tens of meter scale. We use the scheme to record absorption and phase contrast images of a tetra fish, damselfly and yellow jacket, in particular highlighting the contrast enhancement achievable with the simple propagation technique of phase contrast imaging. Coherence and ultrafast pulse duration will allow for the study of various aspects of biomechanics.
Physical Review Special Topics-accelerators and Beams | 2012
S. Kneip; C. McGuffey; J. L. Martins; M. S. Bloom; V. Chvykov; F. Dollar; Ricardo Fonseca; S. Jolly; G. Kalintchenko; K. Krushelnick; A. Maksimchuk; S. P. D. Mangles; Z. Najmudin; C. A. J. Palmer; K. Ta Phuoc; W. Schumaker; L. O. Silva; Jorge Vieira; V. Yanovsky; A. G. R. Thomas
We propose and use a technique to measure the transverse emittance of a laser-wakefield accelerated beam of relativistic electrons. The technique is based on the simultaneous measurements of the electron beam divergence given by v(perpendicular to)/v(parallel to), the measured spectrum gamma, and the transverse electron bunch size in the bubble r(perpendicular to). The latter is obtained via the measurement of the source size of the x rays emitted by the accelerating electron bunch in the bubble. We measure a normalized rms beam transverse emittance <0.5 pi mm mrad as an upper limit for a spatially Gaussian, spectrally quasimonoenergetic electron beam with 230 MeV energy in agreement with numerical modeling and analytic theory in the bubble regime.
Physics of Plasmas | 2008
Anatoly Maksimchuk; Steven A. Reed; Stepan Bulanov; V. Chvykov; G. Kalintchenko; T. Matsuoka; Christopher McGuffey; G. Mourou; Natalia M. Naumova; John A. Nees; P. Rousseau; V. Yanovsky; Karl Krushelnick; Nicholas H. Matlis; Serguei Y. Kalmykov; Gennady Shvets; M. C. Downer; C. R. Vane; James R. Beene; D. W. Stracener; D. R. Schultz
Experiments on electron acceleration and optical diagnostics of laser wakes were performed on the HERCULES facility in a wide range of laser and plasma parameters. Using frequency domain holography we demonstrated single shot visualization of individual plasma waves, produced by 40TW, 30fs laser pulses focused to the intensity of 1019W∕cm2 onto a supersonic He gas jet with plasma densities ne<1019cm−3. These holographic “snapshots” capture the variation in shape of the plasma wave with distance behind the driver, and resolve wave front curvature seen previously only in simulations. High-energy quasimonoenergetic electron beams were generated using plasma density in the range 1.5×1019≤ne≤3.5×1019cm−3. These experiments demonstrated that the energy, charge, divergence, and pointing stability of the beam can be controlled by changing ne, and that higher electron energies and more stable beams are produced for lower densities. An optimized quasimonoenergetic beam of over 300MeV and 10mrad angular divergence i...
Applied Physics Letters | 2009
S. Reed; T. Matsuoka; Stepan Bulanov; M. Tampo; V. Chvykov; G. Kalintchenko; P. Rousseau; V. Yanovsky; R. Kodama; Dale W. Litzenberg; Karl Krushelnick; Anatoly Maksimchuk
A relativistic plasma shutter technique is proposed and tested to remove the sub-100 ps pedestal of a high-intensity laser pulse. The shutter is an ultrathin foil placed before the target of interest. As the leading edge of the laser ionizes the shutter material it will expand into a relativistically underdense plasma allowing for the peak pulse to propagate through while rejecting the low intensity pedestal. An increase in the laser temporal contrast is demonstrated by measuring characteristic signatures in the accelerated proton spectra and directionality from the interaction of 30 TW pulses with ultrathin foils along with supporting hydrodynamic and particle-in-cell simulations.
Journal of Modern Optics | 2005
John A. Nees; Natalia M. Naumova; Erik Power; V. Yanovsky; Igor V. Sokolov; Anatoly Maksimchuk; S.-W. Bahk; V. Chvykov; G. Kalintchenko; B. Hou; G. Mourou
Isolated attosecond pulses and electron bunches can be efficiently generated in the interaction of intense lasers with plasma in the confined volume of the λ3 regime. Scaling with intensity is found to improve pulse brevity and focusability greatly while the efficiency of the attosecond pulse generation continues to remain high. Practical consideration of the tools needed to generate such pulses indicates that such interactions are surprisingly accessible. We mention some introductory experiments whereby we may verify the theoretical predictions of this new class of attosecond pulses. This technique may enable us to reach the Schwinger intensity 1029 W cm−2.
Physics of Plasmas | 2009
C. McGuffey; M. Levin; T. Matsuoka; V. Chvykov; G. Kalintchenko; P. Rousseau; V. Yanovsky; A. Zigler; Anatoly Maksimchuk; Karl Krushelnick
An ablatively driven capillary discharge plasma waveguide has been used to demonstrate guiding of 30 fs, 35 TW laser pulses over distances up to 3 cm with incident intensity in excess of 4×1018 W/cm2. The plasma density range over which good guiding was observed was 1–3×1018 cm−3. The quality of the laser spot at the exit mode was observed to be similar to that at the entrance and the transmitted energy was ∼25% at input powers of 35 TW. The transmitted laser spectrum typically showed blueshifting due to ionization of carbon and hydrogen atoms in the capillary plasma by the high intensity laser pulse. The low plasma density regime in which these capillaries operate makes these devices attractive for use in single stage electron accelerators to multi-GeV energies driven by petawatt class laser systems.
Harnessing Relativistic Plasma Waves as Novel Radiation Sources from Terahertz to X-Rays and Beyond | 2009
S. Kneip; C. McGuffey; S. R. Nagel; C. A. J. Palmer; C. Bellei; J. Schreiber; C. Huntington; F. Dollar; T. Matsuoka; V. Chvykov; G. Kalintchenko; V. Yanovsky; Anatoly Maksimchuk; K. Ta Phuoc; S. P. D. Mangles; K. Krushelnick; Z. Najmudin
The dynamics of relativistic electrons in a laser driven plasma cavity are studied via measurements of their radiation. For ultrashort laser pulses at comparatively low focused laser intensities (3 < a0 < 10), low density and long f-number of 10, electrons are predominantly accelerated in the wakefield leading to quasi-monoenergetic collimated electron beams and well collimated (< 12 mrad) beams of comparatively soft x-rays (1-10 keV) with unprecedented small source size (2-3 μm). For laser pulses with increasing laser intensity (10 < a0 < 30), density and short f-number (< 5), electrons are accelerated directly by the laser, leading to divergent quasimaxwellian electron beams and divergent (50-95°) beams of hard x-rays (20-50 keV) with relatively large source size (> 100 μm). In both cases, the measured x-rays are well described in the synchrotron asymptotic limit of electrons oscillating in a plasma channel. At low laser intensity transverse oscillations are small as the electrons are predominantly accelerated axially by the laser generated wakefield. At high laser intensity, electrons are directly accelerated by the laser. A betatron resonance leads to a tenfold increase in transverse oscillation amplitude and electrons enter a highly radiative regime with up to 5% of their energy converted into x-rays.
Applied Physics Letters | 2006
S. Reed; V. Chvykov; G. Kalintchenko; T. Matsuoka; P. Rousseau; V. Yanovsky; C. R. Vane; James R. Beene; D. W. Stracener; D. R. Schultz; Anatoly Maksimchuk
Recent advancements in laser wakefield accelerators have resulted in the generation of low divergence, hundred MeV, quasimonoenergetic electron beams. The bremsstrahlung produced by these highly energetic electrons in heavy converters includes a large number of MeV γ rays that have been utilized to induce photofission in natural uranium. Analysis of the measured delayed γ emission demonstrates production of greater than 3×105 fission events per joule of laser energy, which is more than an order of magnitude greater than that previously achieved. Monte Carlo simulations model the generated bremsstrahlung spectrum and compare photofission yields as a function of target depth and incident electron energy.
Journal of Applied Physics | 2007
S. Reed; V. Chvykov; G. Kalintchenko; T. Matsuoka; V. Yanovsky; C. R. Vane; J. R. Beene; D. W. Stracener; D. R. Schultz; Anatoly Maksimchuk
Pulses of nearly monoenergetic relativistic electrons have been generated by laser wakefield acceleration and used to perform photonuclear activation of carbon, copper, and photofission in uranium. Using bremsstrahlung converter targets, the electron beams generated by this technique have been shown to be effective in producing high energy γ-rays (tens of MeV) that are necessary to efficiently induce photonuclear reactions. Quantitative γ-ray spectroscopy of the irradiated C, Cu, and U samples indicates that more than 105 reactions were produced per joule of laser energy. The activation yield measurements have been compared with Monte Carlo modeling of electromagnetic cascade and photonuclear processes occurring in the targets to infer the characteristics of the laser accelerated electron beams.
Physics of Plasmas | 2012
C. McGuffey; T. Matsuoka; S. Kneip; W. Schumaker; F. Dollar; C. Zulick; V. Chvykov; G. Kalintchenko; V. Yanovsky; A. Maksimchuk; A. G. R. Thomas; K. Krushelnick; Z. Najmudin
Understanding the scaling of laser wakefield acceleration (LWFA) is crucial to the design of potential future systems. A number of computational and theoretical studies have predicted scalings with laser power for various parameters, but experimental studies have typically been limited to small parameter ranges. Here, we detail extensive measurements of LWFA experiments conducted over a considerable range in power from 20 to 110 TW, which allows for a greater plasma density range and for a large number of data points. These measurements include scalings of the electron beam charge and maximum energy as functions of density as well as injection threshold density, beam charge, and total beam energy as functions of laser power. The observed scalings are consistent with theoretical understandings of operation in the bubble regime.