S. Kar
Queen's University Belfast
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Publication
Featured researches published by S. Kar.
New Journal of Physics | 2008
A. P. L. Robinson; M. Zepf; S. Kar; R. G. Evans; C. Bellei
A new regime is described for radiation pressure acceleration of a thin foil by an intense laser beam of above 1020 W cm−2. Highly monoenergetic proton beams extending to giga-electron-volt energies can be produced with very high efficiency using circularly polarized light. The proton beams have a very small divergence angle (<4°). This new method allows the construction of ultra-compact proton and ion accelerators with ultra-short particle bursts.
Review of Scientific Instruments | 2004
B. Dromey; S. Kar; M. Zepf; P. S. Foster
Plasma mirrors are devices capable of switching very high laser powers on subpicosecond time scales with a dynamic range of 20–30 dB. A detailed study of their performance in the near-field of the laser beam is presented, a setup relevant to improving the pulse contrast of modern ultrahigh power lasers (TW–PW). The conditions under which high reflectivity can be achieved and focusability of the reflected beam retained are identified. At higher intensities a region of high specular reflectivity with rapidly decreasing focusability was observed, suggesting that specular reflectivity alone is not an adequate guide to the ideal range of plasma mirror operation. It was found that to achieve high reflectivity with negligible phasefront distortion of the reflected beam the inequality csΔt<λLaser must be met (cs: sound speed, Δt: time from plasma formation to the peak of the pulse). The achievable contrast enhancement is given by the ratio of plasma mirror reflectivity to cold reflectivity.
Plasma Physics and Controlled Fusion | 2005
M. Koenig; A. Benuzzi-Mounaix; A. Ravasio; T. Vinci; Norimasa Ozaki; S. Lepape; D. Batani; Gael Huser; T. Hall; D. G. Hicks; A. J. Mackinnon; P. K. Patel; H.-S. Park; T. R. Boehly; M. Borghesi; S. Kar; L. Romagnani
In the last few years, high power lasers have demonstrated the possibility to explore a new state of matter, the so-called warm dense matter. Among the possible techniques utilized to generate this state, we present the dynamic compression technique using high power lasers. Applications to planetary cores material (iron) will be discussed. Finally new diagnostics such as proton and hard-x-ray radiography of a shock propagating in a solid target will be presented.
Physical Review Letters | 2008
S. Kar; K. Markey; P.T. Simpson; C. Bellei; J. S. Green; S. R. Nagel; S. Kneip; D. C. Carroll; B. Dromey; L. Willingale; E. L. Clark; P. McKenna; Z. Najmudin; K. Krushelnick; P. A. Norreys; R. J. Clarke; D. Neely; M. Borghesi; M. Zepf
The emission characteristics of intense laser driven protons are controlled using ultrastrong (of the order of 10(9) V/m) electrostatic fields varying on a few ps time scale. The field structures are achieved by exploiting the high potential of the target (reaching multi-MV during the laser interaction). Suitably shaped targets result in a reduction in the proton beam divergence, and hence an increase in proton flux while preserving the high beam quality. The peak focusing power and its temporal variation are shown to depend on the target characteristics, allowing for the collimation of the inherently highly divergent beam and the design of achromatic electrostatic lenses.
Physics of Plasmas | 2009
T. Tanimoto; H. Habara; R. Kodama; M. Nakatsutsumi; K. A. Tanaka; K. L. Lancaster; J. S. Green; R. H. H. Scott; M. Sherlock; P. A. Norreys; R. G. Evans; M. G. Haines; S. Kar; M. Zepf; J. King; T. Ma; Mingsheng Wei; T. Yabuuchi; F. N. Beg; M.H. Key; P.M. Nilson; R. Stephens; H. Azechi; Keiji Nagai; Takayoshi Norimatsu; K. Takeda; J. Valente; J. R. Davies
Fast electron energy spectra have been measured for a range of intensities between 1018 and 1021Wcm−2 and for different target materials using electron spectrometers. Several experimental campaigns were conducted on petawatt laser facilities at the Rutherford Appleton Laboratory and Osaka University, where the pulse duration was varied from 0.5to5ps relevant to upcoming fast ignition integral experiments. The incident angle was also changed from normal incidence to 40° in p-polarized. The results confirm a reduction from the ponderomotive potential energy on fast electrons at the higher intensities under the wide range of different irradiation conditions.
Plasma Physics and Controlled Fusion | 2005
P. K. Patel; M.H. Key; A. J. Mackinnon; R. Berry; M. Borghesi; D. M. Chambers; H. Chen; R. J. Clarke; C. M. Damian; R. Eagleton; R. R. Freeman; S. H. Glenzer; G. Gregori; R. Heathcote; D. Hey; N. Izumi; S. Kar; J. King; A. Nikroo; A. Niles; H.-S. Park; J. Pasley; N. Patel; R. Shepherd; Richard Adolph Snavely; D Steinman; C. Stoeckl; M. Storm; W. Theobald; R. P. J. Town
We review a recent experimental campaign to study the interaction physics of petawatt laser pulses incident at relativistic intensities on solid targets. The campaign was performed on the 500 J sub-picosecond petawatt laser at the Rutherford Appleton Laboratory. An extensive suite of optical, x-ray, and particle diagnostics was employed to characterise the processes of laser absorption, electron generation and transport, thermal and K-alpha x-ray generation, and proton acceleration.
Plasma Physics and Controlled Fusion | 2007
Matthew Zepf; B. Dromey; S. Kar; C. Bellei; D. C. Carroll; R. J. Clarke; J.S. Green; S. Kneip; K. Markey; S. R. Nagel; P.T. Simpson; L. Willingale; P. McKenna; D. Neely; Z. Najmudin; K. Krushelnick; P. A. Norreys
An intense laser pulse interacting with a near discontinuous plasma vacuum interface causes the plasma surface to perform relativistic oscillations. The reflected laser radiation then contains very high order harmonics of fundamental frequency and-according to current theory-must be bunched in radiation bursts of a few attoseconds duration. Recent experimental results have demonstrated x-ray harmonic radiation extending to 3.3 angstrom (3.8 keV, order n > 3200) with the harmonic conversion efficiency scaling as eta(n) n(-2.5) over the entire observed spectrum ranging from 17 nm to 3.3 angstrom. This scaling holds up to a maximum order, n(RO) 81 8(1/2)gamma(3), where gamma is the peak value of the Lorentz factor, above which the harmonic efficiency decreases more rapidly. The coherent nature of the generated harmonics is demonstrated by the highly directional beamed emission, which for photon energy h nu > 1 keV is found to be into a cone angle similar to 4 degrees, significantly less than that of the incident laser cone (20 degrees).
international conference on plasma science | 2009
P. McKenna; D. C. Carroll; Olle Lundh; F. Nürnberg; K. Markey; S. Bandyopadhyay; D. Batani; R. G. Evans; R. Jafer; S. Kar; D. Neely; D. Pepler; M. N. Quinn; R. Redaelli; Markus Roth; C.-G. Wahlstrom; Xiaohui Yuan; M. Zepf
The properties of beams of high energy protons accelerated during ultraintense, picosecond laser-irradiation of thin foil targets are investigated as a function of preplasma expansion at the target front surface. Significant enhancement in the maximum proton energy and laser-to-proton energy conversion efficiency is observed at optimum preplasma density gradients, due to self-focusing of the incident laser pulse. For very long preplasma expansion, the propagating laser pulse is observed to filament, resulting in highly uniform proton beams, but with reduced flux and maximum energy.
2nd International Symposium on Laser-Driven Relativistic Plasmas Applied to Science, Industry and Medicine | 2009
A. S. Pirozhkov; I. W. Choi; J. H. Sung; Soo-Keun Lee; T. J. Yu; T. M. Jeong; I. J. Kim; N. Hafz; C. M. Kim; K. H. Pae; Y.‐C. Noh; D.‐K. Ko; A. P. L. Robinson; P. S. Foster; S. Hawkes; M. Streeter; C. Spindloe; P. McKenna; D. C. Carroll; Claes-Göran Wahlström; M. Zepf; B. Dromey; K. Markey; S. Kar; Y. T. Li; M. H. Xu; H. Nagatomo; M. Mori; Akifumi Yogo; Hiromitsu Kiriyama
High‐power laser contrast is challenging to measure, especially in the real target irradiation conditions. We present a convenient and relatively simple contrast diagnostic technique based on the measurement of target specular reflectivity at full laser power. The reflectivity remains high even at intensities above 1019 W/cm2 in the case of a high‐contrast prepulse‐free laser. On the contrary, the specular reflectivity drops in the case of lower contrast, due to the beam break‐up and increased absorption caused by the preformed plasma. The technique was demonstrated using three different laser systems with several contrast conditions: Astra (CLF, RAL), TiS laser at APRI, GIST, and J‐KAREN (APRC, JAEA).
LASER‐DRIVEN RELATIVISTIC PLASMAS APPLIED FOR SCIENCE, INDUSTRY, AND MEDICINE:#N#The 1st International Symposium | 2008
D. Batani; R. Redaelli; R. Dezulian; Olle Lundh; Filip Lindau; Anders Persson; K. Osvay; C.-G. Wahlstrom; D. C. Carroll; P. McKenna; S. Bandyopadhyay; D. Pepler; D. Neely; S. Kar; P.T. Simpson; K. Markey; Matthew Zepf; M. H. Xu; Y. T. Li
Laser pre‐pulse is a major issue in experiments on laser‐generation of protons, often limiting the performances of laser sources. In this paper, we show how we can actively use a low intensity prepulse (<1013 W/cm2, ns duration) to manipulate the proton beam direction or spatial energy distribution. The prepulse is focused onto the front surface of a thin foil before the arrival of the high intensity pulse (≈1019 W/cm2, ps duration). Under oblique high‐intensity irradiation and for low prepulse intensities, the proton beam is directed away from the target normal. Deviation is towards the laser forward direction, with an angle that increases with the level and duration of the ASE pedestal. Also, for a given laser pulse, beam deviation increases with proton energy. The observations are discussed in terms of Target Normal Sheath Acceleration, in combination with a laser‐controllable shock wave locally deforming the target surface. Results obtained with an annular intensity distribution of the prepulse show s...