Traveling wave tube with gain flattening slow wave structure
    1.
    发明授权
    Traveling wave tube with gain flattening slow wave structure 失效
    具有增益缓慢波浪结构的行驶波浪管

    公开(公告)号:US5162697A

    公开(公告)日:1992-11-10

    申请号:US563582

    申请日:1990-08-06

    IPC分类号: H01J23/24 H01J25/38

    CPC分类号: H01J23/24 H01J25/38

    摘要: A traveling wave tube (10) includes a coupled cavity type slow wave structure (100) having a driver stage (52) and an output section (101) with a primary section (64) and a velocity taper section (82) which in combinattion produce maximum signal gain at a predetermined frequency. A gain flattening section (104) is preferably disposed between the driver stage (52) and the primary section (64) of the output section (101), and is designed to operate at a reduced phase velocity selected to produce minimum or negative signal gain at approximately the predetermined frequency. The gain characteristics of the driver stage (52), gain flattening section (104), primary section (64), and velocity taper section (82) combine to produce minimum signal gain variation over an operating frequency range which spans the predetermined frequency, and expand the bandwidth of the traveling wave tube (10).

    Traveling-wave tube with confined-flow periodic permanent magnet focusing
    2.
    发明授权
    Traveling-wave tube with confined-flow periodic permanent magnet focusing 失效
    具有限流周期性永久磁铁聚焦的行波管

    公开(公告)号:US4942336A

    公开(公告)日:1990-07-17

    申请号:US182632

    申请日:1988-04-18

    IPC分类号: H01J23/06 H01J23/087

    CPC分类号: H01J23/0873 H01J23/06

    摘要: A traveling-wave tube (10) has a confined-flow periodic permanent magnet focusing arrangement (26) in which either the first magnet (60f) or the third magnet (60t) from the electron gun (12) has an extent or axial thickness along the electron stream path which is one-half that of the remaining magnets in the arrangement, thereby providing a scalar magnetic potential of essentially zero on the electron gun pole piece (46), thereby eliminating the field reversal at the cathode (14). This enables a magnetic field to be provided in the region of the electron gun between the gun pole piece (46) and a location behind the cathode due solely to the magnetic field leaking through the gun pole piece aperture (50). The axial magnetic field within the electron gun (12) may be tailored or fine tuned, by varying the size of the aperture (50) in the gun pole piece (46).