High intensity laser generation of proton beams for the production of β+ sources used in positron emission tomography

AIP Conference Proceedings AIP Publishing 584:1 (2001) 73-78

Authors:

I Spencer, KWD Ledingham, RP Singhal, T McCanny, EL Clark, K Krushelnick, M Zepf, FN Beg, M Tatarakis, C Escoda, M Norrefeldt, AE Dangor, PA Norreys, RJ Clarke, RM Allott

Plasma-based studies on 4th generation light sources

AIP Publishing 581:1 (2001) 45-58

Authors:

RW Lee, HA Baldis, RC Cauble, OL Landen, JS Wark, A Ng, SJ Rose, C Lewis, D Riley, J-C Gauthier, P Audebert

Fast heating of ultrahigh-density plasma as a step towards laser fusion ignition.

Nature 412:6849 (2001) 798-802

Authors:

R Kodama, PA Norreys, K Mima, AE Dangor, RG Evans, H Fujita, Y Kitagawa, K Krushelnick, T Miyakoshi, N Miyanaga, T Norimatsu, SJ Rose, T Shozaki, K Shigemori, A Sunahara, M Tampo, KA Tanaka, Y Toyama, T Yamanaka, M Zepf

Abstract:

Modern high-power lasers can generate extreme states of matter that are relevant to astrophysics, equation-of-state studies and fusion energy research. Laser-driven implosions of spherical polymer shells have, for example, achieved an increase in density of 1,000 times relative to the solid state. These densities are large enough to enable controlled fusion, but to achieve energy gain a small volume of compressed fuel (known as the 'spark') must be heated to temperatures of about 108 K (corresponding to thermal energies in excess of 10 keV). In the conventional approach to controlled fusion, the spark is both produced and heated by accurately timed shock waves, but this process requires both precise implosion symmetry and a very large drive energy. In principle, these requirements can be significantly relaxed by performing the compression and fast heating separately; however, this 'fast ignitor' approach also suffers drawbacks, such as propagation losses and deflection of the ultra-intense laser pulse by the plasma surrounding the compressed fuel. Here we employ a new compression geometry that eliminates these problems; we combine production of compressed matter in a laser-driven implosion with picosecond-fast heating by a laser pulse timed to coincide with the peak compression. Our approach therefore permits efficient compression and heating to be carried out simultaneously, providing a route to efficient fusion energy production.

Electron impact excitation of Al XIII : Collision strengths and rate coefficients

The European Physical Journal Special Topics EDP Sciences 11:PR2 (2001) pr2-309-pr2-312

Authors:

KM Aggarwal, FP Keenan, SJ Rose

Electron impact excitation of Gd XXXVII and radiative rates for Ni-like ions with 60 [MATH]

The European Physical Journal Special Topics EDP Sciences 11:PR2 (2001) pr2-313-pr2-316

Authors:

KM Aggarwal, PH Norrington, KL Bell, FP Keenan, GJ Pert, SJ Rose