Abstract:
In an electron gun for use in a TWT, klystron, linear accelerator or other electron device, an electron gun header assembly and an input body assembly are coupled using a flexible bellows that allows the distance between the cathode and anode to be varied. As such, the perveance of the electron gun can be tuned, and the cathode magnetic field optimized for efficient operation. In addition, an external magnetic shield is adapted to be translated along the axial dimension of the electron gun to further optimize the cathode magnetic field and focusing characteristics to achieve improved electron gun performance.

Description:
BACKGROUND OF THE INVENTION 
     1. Field of the Invention 
     The present invention pertains to the field of electron beam tubes and more particularly to an electron gun header having an adjustable perveance that enables the cathode flux to be adjusted and optimized for improved beam focusing. 
     2. Description of Related Art 
     Electron guns are well known and used in standard travelling wave tubes (TWTs), mini-TWTs, klystrons, linear accelerators, and other radio-frequency (RF) electron devices. Such devices typically cause an electron beam originating from an electron gun to propagate through an evacuated tunnel or drift tube that includes an RF interaction structure. The electron beam must be focused by magnetic or electrostatic fields, or both, within the device to minimize beam loss by collision with the walls of the device itself. For example, a TWT operates as a broad-band microwave amplifier that relies on the interaction of a propagating RF wave with the propagating electron beam. In such a tube, the focused electron beam propagates with a velocity slightly faster than that of the RF wave such that the electrons may lose kinetic energy to the wave, thus amplifying its power. Controlling the focusing and propagation of the electron beam is thus important to the performance of the TWT. 
     In a device such as a TWT, the electron beam is formed by an electron gun, which typically comprises an electron-emitting cathode and an anode. The cathode is typically heated to enable thermionic electron emission. When the anode is raised to a potential that is positive with respect to the cathode, the electrons begin to flow as a beam. The geometry of the anode, the cathode, and other focusing electrodes create electromagnetic fields that define the path of the electron beam. In a Pierce gun configuration, the electron beam passes through an opening in the anode to enter the main body of the electron device. In other configurations, a grid is positioned in front of the cathode and affixed to the electrically isolated focus electrode. When the grid is pulsed to a potential sufficiently negative with respect to the cathode, it cuts off the electron current flow and can be used to create a modulated or pulsed electron beam. 
     Many electron guns are designed to exhibit a high perveance, which is defined as the ratio of the space-charge-limited beam current to the gun cathode-to-anode voltage raised to the three halves power. A higher perveance thus indicates that the emitted electron beam is more heavily influenced by space-charge effects. In such a system, the voltage that must be applied to the focus electrode in order to completely cut off the beam current becomes very large. It would thus be beneficial to implement the gun header using a stacked ceramic structure that can support the various elements of the electron gun and also provide a high voltage standoff to support the high voltages necessary to sustain operation at a high perveance. It would also be beneficial to mechanically adjust the perveance of the electron gun and optimize the magnetic flux at the cathode to achieve improved beam focusing. 
     SUMMARY OF THE INVENTION 
     The invention is directed to an electron gun header having an adjustable perveance. In one embodiment of a gun header in accordance with the present invention, a novel vacuum enclosure comprises a stacked ceramic structure to support the structural elements of the electron gun and further to provide a high-voltage standoff to enable operation at voltages substantially higher than those of standard mini-TWT pin-type gun headers. In addition, the gun header includes a bellows assembly and other non-magnetic and magnetic elements that enable the cathode flux to be adjusted and optimized for improved beam focusing and electron gun performance. 
     In one embodiment of a gun header assembly in accordance with the present invention, the gap between the cathode and anode of the electron gun is configured to be mechanically adjustable by the bellows assembly in order to vary the perveance. In addition, magnetic field adjustment in the electron gun region can be accomplished using magnetic elements that are not affixed to the main body of the electron tube. A feature of certain embodiments of the present invention is that during the perveance adjustment process, no magnetic parts are bent or deflected. It is well known in the art that bending magnetic parts can cause work hardening of the material that reduces its ability to support the levels of flux intensity required for good and reliable beam focusing. The perveance adjustment process associated with certain embodiments of the present invention preserves axial alignment between gun elements and maintains azimuthal uniformity of the magnetic field in order to provide excellent beam focusing. 
     In a first embodiment in accordance with the present invention, an electron gun assembly comprises (1) a gun header assembly that includes a cathode adapted to emit an electron beam, wherein the cathode is coupled to a cathode lead connection permitting a cathode voltage bias to be applied to the cathode; a focus electrode fixed in position adjacent to the cathode but electrically isolated from the cathode, wherein the focus electrode is further coupled to a focus electrode lead connection permitting a focus electrode voltage bias to be applied to the focus electrode; and a plurality of ceramic isolating rings fixed in position such that at least one of the plurality of ceramic isolating rings provides electrical isolation between the cathode lead connection and the focus electrode lead connection; and (2) an input body assembly including an anode configured to be adjustably held in place with respect to and in proximity to the cathode and further configured such that an anode voltage potential can be applied to the anode; and a magnetic gun polepiece fixed with respect to the anode but adjustably held in place with respect to the cathode; wherein the input body assembly and the gun header assembly are mechanically coupled using a flexible bellows that enables the input body to be translated axially with respect to the gun header assembly such that a distance between the anode and the cathode and a distance between the magnetic gun polepiece and the cathode can be adjusted. 
     In a preferred embodiment in accordance with the present invention, the flexible bellows is made of a material that is nonmagnetic. In another embodiment in accordance with the present invention, the anode is configured to have a geometry that is substantially ring-shaped, such that the anode includes a central void through which the electron beam can propagate. Such a configuration is known in the art as a Pierce gun configuration. 
     In some embodiments in accordance with the present invention, the cathode is coupled to a cathode heater assembly such that the cathode can be heated to enable thermionic emission. However, a cold-cathode configuration may also be employed and would fall within the scope and spirit of the present invention. 
     In some embodiments in accordance with the present invention, a grid is positioned in front of the cathode and affixed to the electrically isolated focus electrode. In the case of a negative grid gun, the grid may range from a few volts negative with respect to cathode to a potential sufficiently negative with respect to cathode to suppress all emitted current. In the case of an intercepting gridded gun, a similar grid may be pulsed from level of a few hundred volts positive, enabling current flow, to a level a few hundred volts negative, cutting off all current flow. Other arrangements of grids such as shadow grids and tetrode grids may also be employed and would fall within the scope and spirit of the present invention. 
     In some embodiments of an electron gun in accordance with the present invention, the input body further includes a plurality of magnetic polepieces separated by nonmagnetic spacers to form a drift region for the electron beam. The electron gun may also be configured such that the plurality of ceramic isolating rings in the gun header assembly are made from an alumina ceramic material. 
     Further, in some embodiments of an electron gun in accordance with the present invention, the electron gun is surrounded by a nonmagnetic gun shield having a substantially cylindrical shape, such that it substantially encloses the gun header assembly. The electron gun may further include a magnetic flux adjustment shield having a substantially cylindrical shape and located outside of the nonmagnetic gun shield. The magnetic flux adjustment shield is configured such that it can be translated in an axial direction, causing an adjustment of the magnetic field within the gun header region. The adjustment of the magnetic field serves to optimize the cathode flux and electron beam focus. Further, the adjustment of the flexible bellows to alter the distance between the cathode and anode serves to adjust the perveance of the gun assembly. 
     Those skilled in the art will realize other embodiments and applications of the techniques and structures disclosed, and such will also fall within the scope and spirit of the present invention. The invention is described in detail below with reference to the attached sheets of drawings that are first described briefly. In the drawings, reference designators that appear in more than one drawing refer to corresponding physical structures. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG. 1  is a cross section of an electron gun assembly in accordance with an embodiment of the present invention; 
         FIG. 2  is cross section of an input section of an electron gun in accordance with an embodiment of the present invention; 
         FIG. 3  is a three-dimensional drawing of an electron gun and perveance setting fixture in accordance with an embodiment of the present invention; 
         FIG. 4  is a plot of a DEMEOS electrical simulation of an embodiment of an electron gun in accordance with an embodiment of the present invention; 
         FIG. 5  is a plot of the beam filling factor and the tunnel emittance as a function of z-distance along the axis of the electron gun simulation depicted in  FIG. 4 ; 
         FIG. 6  is a DEMEOS simulation plot of an embodiment of an electron gun in accordance with an embodiment of the present invention showing normal beam focusing; 
         FIG. 7  is a DEMEOS simulation plot of an embodiment of an electron gun in accordance with an embodiment of the present invention showing the effect of negative focus electrode voltage on the electron beam; and 
         FIG. 8  is a DEMEOS simulation plot of an embodiment of an electron gun in accordance with an embodiment of the present invention illustrating negative grid cutoff. 
     
    
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
     The invention is directed to an electron gun header having an adjustable perveance.  FIG. 1  is an axial cross section depicting features of an embodiment of an electron gun in accordance with the present invention. Centerline  130  represents the axis of symmetry. The cathode  102  includes a potted heater assembly  112 . One leg of the heater in assembly  112  is connected to the cathode head  102  and the other leg is electrically connected through lead  114  to ribbon  116  to rear flange  128  to cathode end cap  118 . The cathode end cap  118  includes a lead similar to  120  as shown in  FIG. 3  as lead  310 . End cap  118  is sealed to flange  128  by weld joint  142  to produce a hermetic seal to support a vacuum in the gun region. The cathode  102  is mechanically supported near focus electrode  104 . The focus electrode  104  is electrically isolated from the cathode  102  and is coupled to the focus electrode lead  120 . The cathode  102  is electrically connected through metallic structures to a cathode flange lead similar to  120  (rotated in azimuth as shown in  FIG. 3  as lead  320 ). Ceramic rings  110  provide mechanical support and also maintain isolation between the cathode  102  and the focus electrode  104 . In a preferred embodiment, the ceramic rings  110  comprise alumina ceramics, although other materials may also be used. Weld flange  108  is used to connect the gun assembly of  FIG. 1  to the input body assembly depicted in  FIG. 2 , discussed below. Ceramic ring  106  is interposed between the gun assembly of  FIG. 1  and the rest of the input body depicted in  FIG. 2 . 
       FIG. 2  is a cross section of an embodiment of an input section of an electron device in accordance with the present invention. Parts made from magnetic material such as soft iron are shown with dense crosshatching in  FIGS. 1 and 2 . Referring to  FIGS. 1 and 2 , nonmagnetic weld flange  108  is sealed to nonmagnetic ring  204  by weld joint  202  to produce a hermetic seal to support a vacuum in the gun and input section regions. A magnetic gun adjustment disk  206  is supported by nonmagnetic ring  204  and can be used to adjust the focus of the electron beam emitted by the cathode  102 . Magnetic gun polepiece  212  is situated in proximity to the focus electrode  104 , cathode  102 , and anode  214 . Translating the polepiece  212  axially toward or away from cathode  102  changes the focusing behavior of the electron beam. To enable axial movement of the polepiece and anode with respect to the cathode, a flexible bellows  208  is used to attach the magnetic gun adjustment disk  206  and a structural body adjustment disk  210  that is preferably made from a nonmagnetic material. It is preferred that the bellows  208  is made from a nonmagnetic material because it is known in the art that bending of magnetic parts can cause work hardening of the material, which reduces their ability to support sufficient magnetic flux densities to achieve good focusing. Adjusting the distance of the cathode  102  to the anode  214  by flexing the bellows  208  changes the beam current or gun perveance, where perveance is current divided by anode voltage to the 3/2 power. Additional magnetic polepieces  216 , spacers  218 , and ring magnets  230  form part a periodic permanent magnet (PPM) structure used to focus the electron beam downstream within the drift chamber. Although the embodiment depicted in  FIGS. 1 and 2  includes a heated cathode, cold-cathode configurations are also possible, and the perveance-adjusting features of the present invention would apply in the same way to such a configuration. 
     The electron gun and input body structure depicted in  FIGS. 1 and 2 , according to an embodiment of the present invention, thus enable the adjustment of the gun perveance and provide for optimized cathode flux and improved beam focusing. The stacked ceramic structure of the gun allows it to be operated at substantially higher voltages than standard electron gun headers. Adjustment of the spacing between the cathode  102  and anode  214  and magnetic gun polepiece  212  can be accomplished by a setting jig which captures the outer portion of the gun adjustment disk  206  and the outer portion of the structural body adjustment disk  210 . All parts of the setting jig including the screws are made from nonmagnetic materials.  FIG. 3  shows such a setting jig comprised of a body clamp  370  and  371  and gun clamp  360  and  361 . The setting jig includes three push screws  370  and three pull screws  380  that enable the position of cathode  102  to be precisely set with respect to anode  214 . Additional magnetic polepieces, e.g.,  216 , are interposed with non-magnetic spacer rings, e.g.,  218 , along the drift tube. These, along with ring magnets  230  of alternating polarity (not shown in  FIG. 3 ), comprise the PPM focusing structure. 
     Further, in accordance with an embodiment of the present invention,  FIGS. 1 and 3  show a nonmagnetic gun shield  306  surrounded by a magnetic flux adjustment shield  304 . Moving the magnetic flux adjustment shield  304  axially along the gun shield  306  allows for further adjustment of the flux at the cathode for further optimization of the electron beam focusing properties. 
       FIG. 5  depicts the results of an electromagnetic simulation using the DEMEOS electron optics computer code. The geometry of an electron gun in accordance with an embodiment of the present invention is simulated to include a cathode  406  in proximity to a focus electrode  402  and an anode  404 . In this simulation, the cathode  406  is set at a potential of 0 V. Anode  404  is set to V 0  volts, and focus electrode  402  is set at a voltage of −0.00106 times V 0 , just slightly negative with respect to the cathode. A thermal or finite emittance electron beam model is used in the DEMEOS simulations and results of  FIGS. 4 through 8 . Cathode-to-anode voltage, V 0 , ranges from 4 to 8 kV in these plots. However, voltages outside this range can also be applied. In actual guns, the reference for voltage is typically shifted so that the anode is at ground potential or 0 volts and the cathode is at minus V 0 . 
     In  FIG. 4 , Voltage equipotential lines  410  illustrate the simulated electric potential within the gun region. Electrons are drawn from the cathode and are focused into a beam  408  by the electric field between the cathode and the anode and the applied magnetic field  412 . In  FIG. 4 , the level of flux at the cathode has been adjusted by the apparatus and method described above to be 0.63 of the main PPM rms focusing field in accordance with the theory of the inventor. Note that in a PPM focusing system the flux at the cathode can be plus or minus since the value of the B field downstream is sinusoidal. In the case of  FIG. 4 , flux density B at the cathode  406  is negative respect to the first magnetic peak. Further, the value of the first magnetic field peak can be adjusted to achieve an optimal match between the magnetic field at the cathode  406  and the magnetic field downstream. As a result of these adjustments, the focused beam is smooth and of extremely high quality. Note that these results are representative of a particular simulation of a gun header and input section in accordance with the present invention and are meant to be illustrative of gun performance and not limiting in any way. 
       FIG. 5  provides an additional illustration of the performance of the electron gun of  FIG. 4 .  FIG. 5  shows beam filling factor as a function of z distance along the gun axis. The beam filling factor is defined as the 95% beam radius divided by the inner radius of the tunnel through which the beam propagates  440 . In the case of microwave tubes, this tunnel radius is the inner radius of the RF interaction structure. In other words, this metric provides an indication of how well the focusing fields are keeping the electron beam away from the walls of the RF interaction structure. The tunnel emittance  504  is a further measure of beam quality. It is defined as the product of the beam filling factor and the standard deviation of the normalized transverse velocity distribution of the electron beam (parameter sigma). The value of tunnel emittance is quite low in comparison to other guns and beam focusing designs. Further, the model indicates that the emittance is not growing with distance downstream. This is a manifestation of flux at the cathode introduced by the apparatus and methods of this patent. These performance parameters have been achieved by one embodiment of an electron gun in accordance with the present invention. Again,  FIG. 5  is meant to be illustrative of the performance achieved by a particular embodiment of an electron gun in accordance with the present invention and is not intended to be limiting. 
       FIG. 6  depicts an additional DEMEOS electromagnetic simulation of an electron gun header and input section in accordance with an embodiment of the present invention. The geometry of the electron gun and input section is simulated to include alumina ceramic insulators  610 , an electron-emitting cathode  602 , a focus electrode  604 , and an anode  606 . In this simulation, the cathode  602  is held at 0 V, the focus electrode  604  is set just slightly below the cathode potential at −0.00106 times V 0 , and the anode  606  is set to V 0  volts, drawing electrons from the cathode  602 . The resulting electric potential  608  within the gun focuses the electrons into a highly laminar beam  612 . Further inspection of this plot discloses low electrostatic field levels in this configuration resulting in reliable high voltage standoff. Note that the region between the alumna insulators  610  and the nonmagnetic gun shield  620  includes a rubberized potting material which may be Sylgard or other commercially available potting compound. The embodiment depicted in  FIG. 7  also includes this potting material. In  FIGS. 6 and 7 , the heater voltage is −6.3 volts below the potential of the cathode. 
       FIG. 7  depicts an additional DEMEOS simulation of the gun of  FIG. 6  in which the cathode  702  held at a potential of 0 V and the anode  706  at a potential of V 0  volts. However, in this case, the focus electrode  704  has been switched to a potential of −0308 times V 0 , which changes the voltage potential  708  within the gun and partially cuts off the flow of electrons from the cathode. It can be seen that electron flow occurs below the 0 volt equipotential  718  and is completely suppressed above it. The intensity of the electron beam  712  is reduced in comparison to  FIG. 6  and it can be seen that at least a portion of the beam impinges on the anode  706 .  FIGS. 6 and 7  do not include any magnetic focusing field, which is why a portion of the emitted beam is striking the anode. Further, in the gun of  FIG. 7 , if −0360 times V 0  is applied to focus electrode  704 , 100% of the cathode current is suppressed. As in  FIG. 6 , this case illustrates that the electrostatic field levels are also low, resulting in reliable high-voltage standoff. Because the potential of the focus electrode is maximum, referenced to the nonmagnetic gun shield  720 , and the voltage across the gap between the focus electrode  704  and cathode  702  is higher than in the case of  FIG. 6 , it is significant that the design possesses adequate design margin under these conditions. 
       FIG. 8  shows a DEMEOS simulation of a gun with a grid  820  affixed to focus electrode  804  and positioned in front of cathode  802 . When the grid is set to a negative potential with respect to the cathode and equal to the cut off voltage, all electron current from the cathode ceases to flow. The cutoff voltage in this case is −0.088 times V 0 , where V 0  is the applied anode voltage. It can be seen that the 0 volt equipotential  818  is everywhere in front of cathode  802 . Thus, the negative electrostatic fields in front of the cathode suppress all cathode current. In this particular embodiment of an electron gun in accordance with the present invention, the grid thus provides a structure and method of reducing the magnitude of negative voltage required to cut off all beam current. 
     In summary, a robust and high-performance electron gun and input section are disclosed that provide the ability to tune the gun perveance and cathode magnetic field in order to adjust the electron beam focus and device performance. This is accomplished by movement of the anode and magnetic polepiece with respect to the cathode by providing a flexible bellows section that seals the vacuum chamber while allowing for axial translation. Further adjustment of the cathode flux can be accomplished by adjustment of the value of the first magnetic field peak and the adjustment of an external magnetic flux shield. The disclosed configuration has the advantage that no magnetic parts need be bent or flexed in making adjustments to the perveance. This preserves the ability of the magnetic parts to handle large magnetic fluxes necessary for good focusing performance. While the principles and techniques of the present invention are disclosed herein with respect to particular embodiments of an electron gun header and input section, the invention is not limited to the particular configurations discussed. Those skilled in the art will appreciate other embodiments and applications of the novel techniques disclosed herein, and such would also fall within the scope and spirit of the present invention. The invention is further defined by the following claims.