x射线区域的自由电子激光器:量子体制

J. Gea-Banacloche, G. Moore, M. Scully
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摘要

自由电子激光器的量子态定义为:由于有限的相互作用时间,电子在发射光子时损失的能量大于均匀展宽。我们预计,由光波(而不是永磁体摆动器)泵浦的软x射线自由电子激光器将在这种状态下工作。这种情况下的小信号增益由一个明确的量子力学表达式给出。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Free-Electron Lasers in the X-Ray Region: The Quantum Regime
The quantum regime for a free-electron laser is defined as that in which the energy lost by an electron upon emission of a photon is larger than the homogeneous broadening due to the finite interaction time. We anticipate that soft x-ray free-electron lasers pumped by an optical wave (rather than a permanent-magnet wiggler), will operate in that regime. The small-signal gain in this regime is given by an expression which is explicitly quantum-mechanical.
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