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    • 1. 发明授权
    • Rippled beam free electron laser amplifier
    • 起波束自由电子激光放大器
    • US5982787A
    • 1999-11-09
    • US63291
    • 1998-04-21
    • Bruce E. Carlsten
    • Bruce E. Carlsten
    • H01S3/09H01S3/00
    • H01S3/0903
    • A free electron laser amplifier provides a scalloping annular electron beam that interacts with the axial electric field of a TM.sub.0n mode. A waveguide defines an axial centerline and, a solenoid arranged about the waveguide produces an axial constant magnetic field within the waveguide. An electron beam source outputs a annular electron beam that interacts with the axial magnetic field to have an equilibrium radius and a ripple radius component having a variable radius with a ripple period along the axial centerline. An rf source outputs an axial electric field that propagates within the waveguide coaxial with the electron beam and has a radial mode that interacts at the electron beam at the equilibrium radius component of the electron beam.
    • 自由电子激光放大器提供与TM0n模式的轴向电场相互作用的扇形环形电子束。 波导限定轴向中心线,围绕波导管布置的螺线管在波导内产生轴向恒定磁场。 电子束源输出与轴向磁场相互作用以具有平衡半径的环形电子束和具有沿轴向中心线的波动周期的具有可变半径的纹波半径分量。 射频源输出在与电子束同轴的波导内传播的轴向电场,并且具有在电子束的平衡半径分量处与电子束相互作用的径向模式。
    • 2. 发明授权
    • Free electron laser with masked chicane
    • 自由电子激光器与蒙太奇
    • US5956353A
    • 1999-09-21
    • US915235
    • 1997-08-20
    • Dinh C. NguyenBruce E. Carlsten
    • Dinh C. NguyenBruce E. Carlsten
    • H01S3/09H01S3/02
    • H01S3/0903
    • A free electron laser (FEL) is provided with an accelerator for outputting electron beam pulses; a buncher for modulating each one of the electron beam pulses to form each pulse into longitudinally dispersed bunches of electrons; and a wiggler for generating coherent light from the longitudinally dispersed bunches of electrons. The electron beam buncher is a chicane having a mask for physically modulating the electron beam pulses to form a series of electron beam bunches for input to the wiggler. In a preferred embodiment, the mask is located in the chicane at a position where each electron beam pulse has a maximum dispersion.
    • 自由电子激光器(FEL)具有用于输出电子束脉冲的加速器; 用于调制每个电子束脉冲的聚束器,以将每个脉冲形成纵向分散的电子束; 以及用于从纵向分散的电子束产生相干光的摆动器。 电子束聚束器是具有用于物理地调制电子束脉冲以形成一系列用于输入到摆动器的电子束束的掩模的拐角。 在优选实施例中,掩模位于每个电子束脉冲具有最大色散位置的拐角处。
    • 4. 发明授权
    • High brightness electron accelerator
    • 高亮度电子加速器
    • US5336972A
    • 1994-08-09
    • US914327
    • 1992-07-17
    • Richard L. SheffieldBruce E. CarlstenLloyd M. Young
    • Richard L. SheffieldBruce E. CarlstenLloyd M. Young
    • H05H7/22H05H9/00
    • H05H9/00H05H7/22
    • A compact high brightness linear accelerator is provided for use, e.g., in a free electron laser. The accelerator has a first plurality of acclerating cavities having end walls with four coupling slots for accelerating electrons to high velocities in the absence of quadrupole fields. A second plurality of cavities receives the high velocity electrons for further acceleration, where each of the second cavities has end walls with two coupling slots for acceleration in the absence of dipole fields. The accelerator also includes a first cavity with an extended length to provide for phase matching the electron beam along the accelerating cavities. A solenoid is provided about the photocathode that emits the electons, where the solenoid is configured to provide a substantially uniform magnetic field over the photocathode surface to minimize emittance of the electons as the electrons enter the first cavity.
    • 提供紧凑的高亮度线性加速器用于例如自由电子激光器。 加速器具有第一组多个具有四个耦合槽的端壁的积分腔,用于在没有四极场的情况下将电子加速到高速度。 第二多个空腔接收高速电子以进一步加速,其中每个第二腔具有具有两个耦合槽的端壁,用于在没有偶极场的情况下加速。 加速器还包括具有延伸长度的第一腔,以提供沿着加速腔相位匹配电子束。 围绕发射电极的光电阴极设置螺线管,其中螺线管构造成在光电阴极表面上提供基本均匀的磁场,以使电子进入第一腔时的电子发射最小化。
    • 5. 发明授权
    • Stable operating regime for traveling wave devices
    • 行波装置稳定运行方式
    • US6014387A
    • 2000-01-11
    • US915233
    • 1997-08-20
    • Bruce E. Carlsten
    • Bruce E. Carlsten
    • H01S3/09H01S3/00
    • H01S3/0903
    • Autophase stability is provided for a traveling wave device (TWD) electron beam for amplifying an RF electromagnetic wave in walls defining a waveguide for said electromagnetic wave. An off-axis electron beam is generated at a selected energy and has an energy noise inherently arising from electron gun. The off-axis electron beam is introduced into the waveguide. The off-axis electron beam is introduced into the waveguide at a second radius. The waveguide structure is designed to obtain a selected detuning of the electron beam. The off-axis electron beam has a velocity and the second radius to place the electron beam at a selected distance from the walls defining the waveguide, wherein changes in a density of the electron beam due to the RF electromagnetic wave are independent of the energy of the electron beam to provide a concomitant stable operating regime relative to the energy noise.
    • 提供了自相位稳定性,用于在限定用于所述电磁波的波导的壁中放大RF电磁波的行波装置(TWD)电子束。 在所选择的能量下产生离轴电子束,并且具有由电子枪固有地产生的能量噪声。 离轴电子束被引入到波导中。 离轴电子束以第二半径被引入到波导中。 波导结构被设计成获得电子束的选择的失谐。 离轴电子束具有速度和第二半径以将电子束放置在距离限定波导的壁的选定距离处,其中由于RF电磁波而导致的电子束的密度的变化独立于 电子束相对于能量噪声提供相应的稳定操作状态。
    • 6. 发明授权
    • Axial interaction free-electron laser
    • 轴向相互作用的自由电子激光器
    • US5663971A
    • 1997-09-02
    • US626661
    • 1996-04-02
    • Bruce E. Carlsten
    • Bruce E. Carlsten
    • H01S3/09H01S3/00
    • H01S3/0903
    • Electron orbits from a helical axial wiggler in an axial guide field are absolutely unstable as power is extracted from the particles. For off-axis beams an axial FEL mechanism exists when the axial electric field in a TM mode is wiggled to interact with the axial velocity of the electrons that form the beam. The interaction strength is comparable to that for helical FELs and is insensitive to beam orbit errors. The orbits for this mechanism are extremely stable in the absence of space charge and lead to high extraction efficiencies without particle phasing incoherence or interception. This interaction mechanism is suitable for use with intense annular electron beams for high power generation at microwave frequencies.
    • 从轴向导向场中的螺旋轴向摆动器的电子轨道绝对不稳定,因为从颗粒中提取功率。 对于离轴光束,当TM模式的轴向电场被摆动以与形成光束的电子的轴向速度相互作用时,存在轴向FEL机制。 相互作用强度与螺旋FEL的相互作用强度相当,对光束轨道误差不敏感。 这种机制的轨道在没有空间电荷的情况下非常稳定,并导致高提取效率,而没有粒子相位不连续或截取。 这种相互作用机制适用于在微波频率下高功率发射的强环形电子束。