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Plasma accelerators in the 1000 GHz regime; electromagnetic-beat- and beam-driven structures

机译:1000 GHz条件下的等离子加速器;电磁拍和光束驱动的结构

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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.
机译:仅提供摘要表格。接近光速的电子等离子体波(EPW);即,具有与其相速度/ spl Gt / 1相关的洛伦兹因子的EPW,可能成为科学/工业有用的粒子加速结构。加速场E / sub z /可以超过/ spl sim / 10 GHz铜结构中的/ spl sim / 200 MeV / m击穿极限,数量级高。随着EPW频率/ spl nu // sub p /(通过增加等离子体密度n / sub e /)的升高,波长/ splλ// sub p / / spl ap / c // spl nu // sub p /变得更小,大于10 / sup 18 / cm / sup -3 /> 35 / spl mu / m,与传统直线加速器的最短电子束长度相当。当待加速光束的直径为/ spl sim / 10 / spl mu / m时,E / sub z /的横向变化以及固有的强聚焦场E / sub r /的重要性也对密度施加了上限。 ,又是典型的直线加速器。许多短脉冲,激光驱动的等离子体加速器实验,例如Laser Wakefield Accelerator(LWFA),在高于10 / sup 18 / cm / sup -3 /的条件下运行,但通常设想不是通过外部直线加速器而是通过强迫(使用激光的另一支臂)一些等离子体电子离开热分布并被EPW加速。在这些较高的/ spl nu // sub p /实验中,这种电子“注入”方法是必需的,因为“匹配”到EPW中的电子束在所有尺寸上都比从直线加速器所能达到的小得多。本文讨论了两组在1000 GHz频率下产生和使用EPW的实验。首先是在加州大学洛杉矶分校的等离子搏动波加速器(PBWA)实验,其次是在斯坦福线性加速器中心进行的等离子韦克菲尔德加速器(PWFA)实验。在这两种情况下,加速束都是由直线加速器产生的,因此是通过测量EPW引起的对横向尺寸和束能量的修改,E / sub z /(r,z,t)和E / sub r /的某些特性而产生的。 (r,z,t)可以推断出来并与理论进行比较。

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