2006
DOI: 10.1088/0741-3335/48/2/l01
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Observation of annular electron beam transport in multi-TeraWatt laser-solid interactions

Abstract: Electron energy transport experiments conducted on the Vulcan 100 TW laser facility with large area foil targets are described. For plastic targets it is shown, by the plasma expansion observed in shadowgrams taken after the interaction, that there is a transition between the collimated electron flow previously reported at the 10 TW power level to an annular electron flow pattern with a 20 • divergence angle for peak powers of 68 TW. Intermediate powers show that both the central collimated flow pattern and th… Show more

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Cited by 37 publications
(33 citation statements)
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“…1(d) indicates a divergence angle of 10 -25 for those energetic electrons (> 10 MeV) contributing to SPR generation. This is consistent with that (typically 10 -30 )of laser-accelerated hot electrons in overdense plasmas and can be attributed to the confinement effect of the selfgenerated magnetic fields [6,7].…”
supporting
confidence: 89%
“…1(d) indicates a divergence angle of 10 -25 for those energetic electrons (> 10 MeV) contributing to SPR generation. This is consistent with that (typically 10 -30 )of laser-accelerated hot electrons in overdense plasmas and can be attributed to the confinement effect of the selfgenerated magnetic fields [6,7].…”
supporting
confidence: 89%
“…Close to the critical layer, the density is highly modulated at the laser wavelength, and at higher densities it is expelled forming a channel. The electron heat flux in the forward direction is shown to exhibit an annular structure, indicating that, due to the tight focus of the laser, most of fast electrons are accelerated at an angle, which is consistent with experimental observations of annular patterns at the back of a solid target after being hit by an ultraintense laser pulse [8]. The plasma electron kinetic energy is maximum at the tip of the laser pulse where considerable electron acceleration occurs.…”
supporting
confidence: 83%
“…(10) By the way of substituting expressions (1) and (2), which are obtained for the AM fields in the region R 1 < r < R 2 into the Equation (8), one can drive the following equations for derivatives of radial v j and azimuthal u j components of the impulse for j-th particle of the beam over time (meaning of the index j possess the value from 1 until N ): (12) here R 1j = r j R −1…”
Section: Basic Equationsmentioning
confidence: 99%
“…Solution of the set of equations for amplitude (6) and phase (7) of the AMs envelope, motion equations for the beams' electrons (10)- (12) has been found by the Runge-Kutta method of the fourth order, which is widely used for the research of such problems [1,2,14,15]. Quantity of the beams' macro -particles was assumed to be here N = 2000.…”
Section: But Really It Is a Non-linear Condition Because Expression mentioning
confidence: 99%
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