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    • 1. 发明授权
    • Linear accelerator
    • 线性加速器
    • US06710557B1
    • 2004-03-23
    • US10049352
    • 2002-02-05
    • John AllenLeonard Knowles BrundleTerry Arthur LargeTerence Bates
    • John AllenLeonard Knowles BrundleTerry Arthur LargeTerence Bates
    • H01J2510
    • H05H9/04H05H7/18
    • An accelerator comprises a plurality of accelerating cells arranged to convey a beam, adjacent cells being linked by a coupling cell, the coupling cells being arranged to dictate the ratio of electric field in the respective adjacent accelerating cells, at least one coupling cell being switchable between a positive ratio and a negative ratio. Such an accelerator in effect inserts a phase change into the E field by imposing a negative ratio, meaning that the beam will meet a reversed electric field in subsequent cells and will in fact be decelerated. As a result, the beam can be developed and bunched in early cells while accelerating to and/or at relativistic energies, and then bled of energy in later cells to bring the beam energy down to (say) between 100 and 300 KeV. Energies of this magnitude are comparable to diagnostic X-rays, where much higher contrast of bony structures exists. Hence the accelerator can be used to take kilovoltage portal images.
    • 加速器包括多个加速单元,其被布置成传送波束,相邻单元由耦合单元链接,所述耦合单元布置成指示相应相邻加速单元中的电场的比率,至少一个耦合单元可在 正比率和负比率。 这样的加速器实际上通过施加负比率将相位插入到E场中,这意味着光束将在随后的单元中遇到反向的电场,并且实际上将被减速。 结果,可以在加速到和/或相对论能量的同时在早期的单元中显影和聚束光束,然后在稍后的单元中排出能量,以将光束能量降低到(例如)100和300KeV之间。 这种量级的能量与诊断X射线相当,骨骼结构的对比度高得多。 因此,加速器可用于采取千伏门户图像。
    • 2. 发明授权
    • Linear accelerator
    • 线性加速器
    • US06376990B1
    • 2002-04-23
    • US09529757
    • 2000-04-18
    • John AllenLeonard Knowles BrundleTerry Arthur LargeTerence Bates
    • John AllenLeonard Knowles BrundleTerry Arthur LargeTerence Bates
    • H01J2510
    • H05H9/04H05H7/18
    • This device allows the variation of the coupling between two points in an RF circuit in a very simple way while maintaining the RF phase relationship and varying the relative magnitude of the RF fields. The device is characterized by a simple mechanical control of coupling value, that has negligible effect on the phase shift across the device. This is achieved by the simple rotation of the polarisation of a TE111 mode inside a cylindrical cavity. Such a device does not contain resistive elements, and the sliding mechanical surfaces are free from high RF currents. This device finds an application in standing wave linear accelerators, where it is desirable to vary the relative RF field in one set of cavities with respect to another, in order that the accelerator can operate successfully over a wide range of energies.
    • 该装置允许以非常简单的方式在RF电路中的两个点之间的耦合的变化,同时保持RF相位关系并改变RF场的相对幅度。 该器件的特征在于耦合值的简单机械控制,对于跨器件的相移具有可忽略的影响。 这通过在圆柱形腔内的TE111模式的极化的简单旋转来实现。 这种装置不包含电阻元件,并且滑动机械表面没有高RF电流。 该装置在驻波线性加速器中发现了一种应用,其中期望相对于另一组空腔改变相对RF场,以便加速器能够在宽范围的能量范围内成功地运行。
    • 3. 发明授权
    • Linear accelerator
    • 线性加速器
    • US06642678B1
    • 2003-11-04
    • US10049426
    • 2002-02-05
    • John AllenLeonard Knowles BrundleTerry Arthur LargeTerence Bates
    • John AllenLeonard Knowles BrundleTerry Arthur LargeTerence Bates
    • H05H900
    • H05H9/04H05H7/18
    • A standing wave linear accelerator has a plurality of resonant cavities located along a particle beam axis. One or more pairs of resonant cavities are electromagnetically coupled via a coupling cavity. A rotationally asymmetric element within the coupling cavity is adapted to rotate about an axis that is substantially parallel to the axis of the coupling cavity. The coupling cavity is imperfectly symmetric about its axis due to a relative excess of material disposed within the cavity in the portion opposed to the apertures. Rotation of the polarization of a TE111 mode inside the cylindrical cavity provided a simple single mechanical control of coupling value, that has negligible effect on the phase shift across the device. A slight frequency dependence on the angle of rotation is correctable by a relative excess of material located opposite the apertures between the coupling cavity and the accelerating cavities.
    • 驻波直线加速器具有沿着粒子束轴定位的多个谐振腔。 一对或多对谐振腔通过耦合腔电磁耦合。 耦合空腔内的旋转非对称元件适于围绕基本上平行于耦合腔的轴线的轴线旋转。 由于在与孔相对的部分中设置在腔内的材料的相对过量,耦合空腔的轴线不完全对称。 在圆柱形腔内旋转TE111模式的极化提供了耦合值的简单单一机械控制,对整个装置的相移影响可以忽略不计。 通过与耦合腔和加速腔之间的孔相对定位的相对过量的材料可以校正对旋转角度的轻微的频率依赖性。