Title :
Plasma accelerators in the 1000 GHz regime; electromagnetic-beat- and beam-driven structures
Author :
Clayton, C.E. ; Filip, C.V. ; Joshi, C. ; Marsh, K.A. ; Musumeci, P. ; Narang, Rakhi ; Pellegrini, C. ; Rosenzweig, J.B. ; Tochitsky, S.Y. ; Yoder, R.B. ; Barnes, C.D. ; Blue, B.E. ; Decker, F.-J. ; Deng, Shaozhi ; Emma, Philip ; Hogan, M.J. ; Huang, Chao
Author_Institution :
Dept. of Electr. Eng., California Univ., Los Angeles, CA, USA
Abstract :
Summary form only given. A nearly light-speed electron plasma wave (EPW); i.e., an EPW with the Lorentz factor associated with its phase velocity /spl Gt/1, may become a useful particle accelerating structure for science/industry. The accelerating fields E/sub z/ can exceed the /spl sim/200 MeV/m breakdown limit in /spl sim/10 GHz copper structures by orders of magnitude. As one goes up in EPW frequency /spl nu//sub p/ (by increasing the plasma density n/sub e/), the wavelength /spl lambda//sub p/ /spl ap/c//spl nu//sub p/ becomes smaller and above 10/sup 18/ cm/sup -3/ is <35 /spl mu/m, comparable to the shortest electron bunch lengths available from conventional linacs. The transverse variations of E/sub z/ and the importance of the inherent, strong focusing fields E/sub r/ also imposes an upper limit in density when the beam to be accelerated is /spl sim/10 /spl mu/m in diameter, again typical of a linac. Many short-pulse, laser-driven plasma accelerator experiments, such as the Laser Wakefield Accelerator (LWFA), are operated above 10/sup 18/ cm/sup -3/, but often envision creating bunches not from an external linac, but by coercing (using another arm of the laser) some of the plasma electrons to leave the thermal distribution and be accelerated by the EPW. Such an approach to electron "injection" is necessary in these high /spl nu//sub p/ experiments since the beam that "match" into the EPW is much smaller in all dimensions than is achievable from a linac. This paper deals with two sets of experiments that produce and use EPWs in the 1000 GHz regime. First are the Plasma Beatwave Accelerator (PBWA) experiments at UCLA and second are the Plasma Wakefield Accelerator (PWFA) experiments carried out at the Stanford Linear Accelerator Center. In both cases, the accelerated bunch is produced by a linac and thus by measuring the EPW-induced modifications to the transverse size and beam energy, some properties of E/sub z/(r, z, t) and E/sub r/(r, z, t) can be inferred- and compared to theory.
Keywords :
linear accelerators; particle beam bunching; particle beam injection; plasma accelerators; plasma density; plasma waves; wakefield accelerators; 1000 GHz; Lorentz factor; copper structure; electron bunch; electron injection; laser wakefield accelerator; light-speed electron plasma wave; linac; particle accelerator; phase velocity; plasma accelerator; plasma beatwave accelerator; plasma density; plasma electrons; plasma wakefield accelerator; thermal distribution; Acceleration; Electrons; Laser beams; Linear accelerators; Linear particle accelerator; Particle beams; Plasma accelerators; Plasma measurements; Plasma properties; Plasma waves;
Conference_Titel :
Plasma Science, 2004. ICOPS 2004. IEEE Conference Record - Abstracts. The 31st IEEE International Conference on
Conference_Location :
Baltimore, MD, USA
Print_ISBN :
0-7803-8334-6
DOI :
10.1109/PLASMA.2004.1339696