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    • 2. 发明授权
    • Low-power wide-bandwidth klystron
    • 低功率宽带速调管
    • US06326730B1
    • 2001-12-04
    • US09193644
    • 1998-11-16
    • Robert Spencer Symons
    • Robert Spencer Symons
    • H01J2510
    • H01J25/10
    • A low-power wide-bandwidth klystron comprises a cathode having an electron emitting surface capable of emitting an electron beam and a collector spaced from said cathode and designed to collect the electron beam emitted from the cathode. An anode is disposed between the cathode and the collector in order to channel the electron beam into a series of drift tubes that define the electron beam path between the anode and the collector. The drift tubes define gaps in which the input cavity and output cavity interact with the electron beam. The input cavity velocity modulates the electron beam by way of a radio frequency input signal and the output cavity extracts the amplified radio frequency signal from the electron beam. The drift tubes may define additional gaps between the input cavity and output cavity for intermediate cavities that would provide additional amplification. A voltage potential, positive with respect to the cathode voltage potential, is applied to the anode in order to draw the electron beam from the emitting surface of the cathode and into the drift tubes. The anode voltage potential is much larger than required for the desired output power. The output cavity is overloaded by providing it with a load conductance that is at least twice that required for optimal klystron power output. A voltage potential, positive with respect to the cathode voltage potential, is applied to the collector, but the voltage potential difference between the cathode and the collector may be at most one half of a corresponding voltage potential difference between the cathode and the anode.
    • 低功率宽带速调管包括具有能够发射电子束的电子发射表面的阴极和与所述阴极隔开的集电体,并设计成收集从阴极发射的电子束。 阳极设置在阴极和收集器之间,以便将电子束传送到一系列漂移管中,该漂移管限定了阳极和收集器之间的电子束路径。 漂移管限定了输入腔和输出腔与电子束相互作用的间隙。 输入腔速度通过射频输入信号调制电子束,输出腔从电子束中提取放大的射频信号。 漂移管可以在输入腔和输出腔之间形成额外的间隙,用于提供额外放大的中间腔。 将相对于阴极电压电位为正的电压电位施加到阳极,以便从阴极的发射表面吸引电子束并进入漂移管。 阳极电压电位远大于所需输出功率所需的电压。 输出腔通过为其提供至少为最佳速调管功率输出所需的两倍的负载电导而过载。 对集电极施加相对于阴极电压电位为正的电压电位,但是阴极和集电极之间的电压电位差可以是阴极和阳极之间的相应电压电位差的至多一半。
    • 8. 发明授权
    • Cathode ray tube with efficiently driven electron gun
    • 具有高效驱动电子枪的阴极射线管
    • US06768267B2
    • 2004-07-27
    • US10253605
    • 2002-09-25
    • Woo-seok HuhMin-cheol Bae
    • Woo-seok HuhMin-cheol Bae
    • H01J2510
    • H01J29/485H01J2229/4841H01J2229/4844
    • A cathode ray tube (CRT) has an electron gun including a cathode for emitting electron beams, a control electrode for controlling emission of the electron beams from the cathode, and a screen electrode for accelerating the flow of the electron beams passing the control electrode are arranged in series. In the CRT, during a scanning period, a voltage applied to at least one of the control electrode and the screen electrode changes in response to a voltage of a data signal applied to the cathode. The control electrode and screen electrode each include three mutually electrically insulated sections for independently controlling each of three electron beams passing through the electrodes.
    • 阴极射线管(CRT)具有包括用于发射电子束的阴极的电子枪,用于控制来自阴极的电子束发射的控制电极和用于加速通过控制电极的电子束流动的屏幕电极 串联排列。 在CRT中,在扫描期间,施加到控制电极和屏幕电极中的至少一个的电压响应于施加到阴极的数据信号的电压而改变。 控制电极和屏幕电极各自包括三个相互电绝缘的部分,用于独立地控制通过电极的三个电子束中的每一个。
    • 9. 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。