EP3007199A1 - Dispositif de tube à électrons - Google Patents

Dispositif de tube à électrons Download PDF

Info

Publication number
EP3007199A1
EP3007199A1 EP14003487.7A EP14003487A EP3007199A1 EP 3007199 A1 EP3007199 A1 EP 3007199A1 EP 14003487 A EP14003487 A EP 14003487A EP 3007199 A1 EP3007199 A1 EP 3007199A1
Authority
EP
European Patent Office
Prior art keywords
electron
tube device
gate electrode
collector
electrode
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
EP14003487.7A
Other languages
German (de)
English (en)
Inventor
Jochen Mannhart
Cyril STEPHANOS
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Max Planck Gesellschaft zur Foerderung der Wissenschaften eV
Original Assignee
Max Planck Gesellschaft zur Foerderung der Wissenschaften eV
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Max Planck Gesellschaft zur Foerderung der Wissenschaften eV filed Critical Max Planck Gesellschaft zur Foerderung der Wissenschaften eV
Priority to EP14003487.7A priority Critical patent/EP3007199A1/fr
Publication of EP3007199A1 publication Critical patent/EP3007199A1/fr
Withdrawn legal-status Critical Current

Links

Images

Classifications

    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J3/00—Details of electron-optical or ion-optical arrangements or of ion traps common to two or more basic types of discharge tubes or lamps
    • H01J3/02—Electron guns
    • H01J3/027—Construction of the gun or parts thereof
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J29/00—Details of cathode-ray tubes or of electron-beam tubes of the types covered by group H01J31/00
    • H01J29/46—Arrangements of electrodes and associated parts for generating or controlling the ray or beam, e.g. electron-optical arrangement
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J29/00—Details of cathode-ray tubes or of electron-beam tubes of the types covered by group H01J31/00
    • H01J29/46—Arrangements of electrodes and associated parts for generating or controlling the ray or beam, e.g. electron-optical arrangement
    • H01J29/48—Electron guns
    • H01J29/485—Construction of the gun or of parts thereof
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J2203/00—Electron or ion optical arrangements common to discharge tubes or lamps
    • H01J2203/02—Electron guns
    • H01J2203/0204—Electron guns using cold cathodes, e.g. field emission cathodes
    • H01J2203/0208—Control electrodes
    • H01J2203/0212—Gate electrodes
    • H01J2203/0232—Gate electrodes characterised by the material

Definitions

  • the present invention relates to an electron tube device comprising at least one electron emitter, at least one electron collector and at least one gate electrode.
  • the electron tube device is adapted for controlling electric current between the at least one electron emitter and at least one of the at least one electron collector and the at least one gate electrode.
  • the present invention relates to a method of controlling electric current, wherein the electron tube device is used. Applications of the invention are available in the fields of actively controlling electric currents, or operating display devices.
  • Electron tubes are active electronic components, which are used for e. g. the generation, amplification, rectification, modulation and/or control of electric current. Typical applications are known in the fields of radar and radio technique, magnetrons, plasma generation, X-ray generation (X-ray tubes), cathode ray generation (cathode ray tube, e. g. in an oscilloscope) or vacuum fluorescence displays.
  • a conventional electron tube 100' comprises an electron emitter 10' (cathode), an electron collector 20' (anode) and a gate electrode 30' in a vessel 60', which is evacuated or filled with a working gas (see Figure 7 , prior art). Electrons are created at the electron emitter 10' e. g. by thermoionic emission from a hot filament or a cathode 11' indirectly heated with a heater filament 13'.
  • the gate electrode 30' is connected with a gate voltage source 32'. The electric current through the electron tube 100' can be controlled in dependency on the voltage Vg of the gate voltage source 23'.
  • the voltage Vg generally is a negative voltage relative to the emitter electrode 10', or with special applications (so called "space charge grids") a positive voltage can be used.
  • space charge grids special applications
  • multiple gate electrodes 30' can be provided, which are connected with specific voltage sources.
  • Space charges which are created at the electrodes and in the space between the electrodes, reduce the current between the electron emitter 10' and the electron collector 20', thus restricting the efficiency of the tube operation.
  • a positive voltage Va can be applied to the electron collector 20'.
  • the positive voltage Va increases the current density.
  • an undisred increase of dissipation loss is created simultaneously.
  • the effect of the space charges and dissipation losses could be reduced by a longitudinal magnetic field between the electron emitter 10' and the electron collector 20' in combination with a positive gate voltage Vg, as it is known from thermoelectronic generators [1-4].
  • Vg positive gate voltage
  • the effect of the space charges can be substantially reduced and increased current densities could be obtained even at a relatively low gate voltage (e. g. ⁇ 20 V).
  • creating the magnetic field with a sufficient field strength represents a disadvantage for most of the applications of electron tubes.
  • single electronic tubes being adapted for creating the magnetic field would have a complex structure and increased size.
  • the range of available materials of the remaining tube components is restricted as the remaining components should not include magnetic materials.
  • the gate electrode 30' is a grid electrode made of filaments forming a lattice, wherein the electrons pass the meshes of the lattice.
  • C. Li et al. have proposed a field emission triode tube with a gate electrode made of graphene (see [8]).
  • Graphene forms a continuous membrane-shaped layer, which is semi-transparent for the electrons.
  • the electrons pass the layer material as such.
  • gate electrodes can be made of carbon nano-tubes (see [11-13]).
  • nano-tube based gate electrodes have disadvantages in terms of an inhomogeneous density and electron transmission in longitudinal direction (perpendicular to the emitter and collector surfaces) and a complex manufacturing process.
  • the objective of the present invention is to provide an improved electron tube device, which is capable of avoiding disadvantages and limitations of conventional electron tubes. It is a particular objective of the invention to provide the electron tube device having reduced dissipation losses, increased current density, reduced weight and size, reduced costs, improved operation efficiency, and/or improved variability in terms of materials for manufacturing the electron tube. It is a further objective of the invention to provide an improved method of controlling an electric current using an electron tube.
  • an electron tube device which comprises an electron emitter (cathode), an electron collector (anode) and a gate electrode.
  • the electron tube device is a vacuum tube (valve) for the generation, amplification, rectification, modulation and/or control of electric current.
  • the electron emitter and the electron collector are arranged with a mutual gap (spacing), wherein emitter and collector surfaces point to the gap, resp..
  • the electron collector preferably is made of a material having a work function, which is larger compared with the work function of the electron emitter material.
  • the electron emitter is adapted for a release of electrons by direct heating (thermoionic emission) or indirect heating and the effect of an accelerating voltage applied to the electron tube.
  • the electron collector is adapted for a collection of the electrons.
  • the gate electrode is arranged between the electron emitter and the electron collector for subjecting the electrons emitted from the electron emitter to an electrical potential, e. g. a negative potential, an electron accelerating electrical potential, an alternating potential and/or a switched potential sequence.
  • the gate electrode comprises at least one membrane-shaped, electrically conductive or semiconductive electrode layer, which is at least partially transparent for the electrons (semi-transparent electrode layer).
  • the at least one membrane-shaped, partially or completely transparent electrode layer (or: electrode layer) is capable of creating the electric field, while the electrons can pass the gate electrode material.
  • a free-standing thin membrane of a material with electron transmission (or low electron absorption) can be passed by the electrons with only small or negligible energy loss, so that it can be used as a homogeneous, negatively or positively charged gate electrodes.
  • the material and/or thickness of the at least one electrode layer are selected such that electrons traveling towards the collector electrode are transmitted through the layer material, i.e. the electrons pass through a continuous section of the material layer. The electrons pass through the layer material as such.
  • the at least one electrode layer is partially transparent, i.e. it has at least 20 %, preferably at least 25 %, particularly preferred at least 50 % electron transmission probability.
  • the at least one membrane-shaped, partially transparent electrode layer consists of a two-dimensional material (graphene-like material). Particularly preferred, the two-dimensional material is at least one atomic monolayer.
  • the at least one electrode layer of the gate electrode has a plurality (at least two) through-holes and/or includes at least one dopant.
  • the through-holes are openings in the at least one electrode layer.
  • the electrode layer is formed as a grid, e. g. a regular or irregular grid.
  • the regular grid is a hexagonal grid.
  • the through-holes may have a circular or non-circular, e. g. elliptic, rectangular or triangular shape.
  • the dopant is a substance included in the material of the at least one electrode layer, wherein the dopant has an electron absorption reducing effect, in particular by changing the Fermi energy of the layer material and/or a reduction of energy losses by adjusting a plasmon frequency in the layer material.
  • conductive or semiconductive, two-dimensional materials like graphene or graphene-like materials, have further advantages as they allow a reduction of electron absorption by changing the Fermi energy of the layer material and/or a reduction of energy losses by adjusting a plasmon frequency in the layer material by adding the at least one dopant (at least one doping substance) to the layer material.
  • the doping allows a shifting of the Fermi energy (see e.g. [6, 7]), so that the absorption of electrons can be reduced, in particular in predetermined electron energy intervals.
  • this conduction can be enhanced by doping the two-dimensional material or by adding one or more ultrathin conducting layers onto the two-dimensional material.
  • the electrons pass graphene or similar materials, they can excite plasmons, thus losing energy.
  • the plasmon frequency e.g. in graphene, can be changed by doping, so that energy losses of the electrons are reduced.
  • an increased electron transmission probability can be obtained compared e. g. with the graphene gate of [8] as the electron absorption is further reduced by the through-holes and/or doping, while the mechanical stability of the at least one electrode layer is kept.
  • the electrons pass through the layer material of the at least one electrode layer or through the holes.
  • the efficiency of the current control with the electron tube can be improved.
  • the invention proposes new electron tubes with reduced volume, weight and material requirements. Moving or vibrating mechanical parts are avoided, so that the inventive electron tube device is capable of a noise-free and vibration-free operation. As the electron tube device does not require external magnetic fields, the creation of magnetic stray fields is avoided.
  • the electron tube device preferably is at least one of an active electronic component for current rectification, an active electronic component for current modulation and/or control, a vacuum fluorescence display, an active electronic component for ignition voltage reduction in fluorescent tubes, and an ion source.
  • the at least one electrode layer may include at least 10 through-holes, preferably at least 100 through-holes, e. g. 1000 through-holes or more distributed over the area of the at least one electrode layer facing to the electron emitter.
  • the total area of the through-holes may be at least 10 %, preferably at least 20 %, particularly preferred at least 40 %, e. g. 60 % or more, of an exposed surface of the gate electrode facing to the electron emitter.
  • the inventors have found that the number of electrons reaching the electron collector continuously increases as a function of decreasing hole diameter with constant gate electrode transparency (area of through-holes / area of the gate electrode) if the diameter of the holes is small compared with the distance between the electron emitter and the electron collector.
  • the hole diameter With reducing the hole diameter, the homogeneity of the electric field is improved as transversal field components are reduced. Accordingly, a transversal deflection of electrons is reduced, thus decreasing the electron absorption at the gate electrode and increasing the electron current to the electron collector.
  • the cross-sectional dimension, like the hole diameter, of the through-holes can be selected to be smaller than 500 ⁇ m, in particular smaller than 200 ⁇ m.
  • a hole diameter below 10 ⁇ m in particular below 5 ⁇ m, e. g. 1 ⁇ m
  • the inventors have found that e. g. a structured graphene grid with a hole diameter of 1 ⁇ m and a lateral width of the layer sections between the holes of 5 nm has an electron absorption below 1 %. In particular this low electron absorption allows to omit a magnetic field, thus clearly showing the advantage compared with the conventional techniques.
  • the through-holes can be created e.g. with electron beam lithography or optical lithography, combined with ion etching or chemical etching.
  • An irregular grid of through-holes can be made e. g. by ion irradiation.
  • the inventive gate electrode has an improved homogeneity and planarity.
  • Graphene and similar materials can be structured easily, e.g. by electron beam lithography.
  • the inventive gate electrodes allow the provision of three electrodes electron tubes, in particular with minimized size and weight, having an emitter-collector-distance below 10 ⁇ m, in particular below 5 ⁇ m. This distance cannot be obtained with conventional, grid-based gate electrodes, as the electric field in the lattice meshes would be very small, if the emitter-gate-distance would be substantially larger than the mesh diameter.
  • current densities of some A/cm 2 can be obtained by suppressing space charge effects. Contrary to semiconductor transistors, electron transport in electron tubes is a ballistic transport, and the heat transport is essentially reduced. Furthermore, a positive gate voltage in combination with low losses at the gate electrode offers the possibility to use field emission at the emitter, wherein a field strength of about 10 6 V/m is used for Schottky field emission, or a field strength above 10 9 V/m is used for Fowler-Nordheim emission. With an emitter-gate distance of about 100 ⁇ m, a gate voltage below 100 V, in particular below 10 V could be used for field emission.
  • the gate dissipation loss can be drastically reduced compared with conventional field emission triodes.
  • the gate voltage necessary for Schottky or Fowler-Nordheim field emission can be reduced by using an emitter provided with nanotubes, exploiting the strong electric field at the tips of the nanotubes.
  • the electron emitter and collector electrodes can be provided as filaments, plates or membranes spaced from each other, in particular having a linear or planar shape.
  • the gate electrode may be provided, e. g. manufactured or deposited, on the emitter or on the collector electrode, provided it is electrically insulated from the emitter or collector electrode.
  • the membrane structure of the electrodes allows the construction of the electron tube device with a compact structure.
  • the emitter and collector electrodes also may comprise thin films, foils, or membranes, the weight and/or the material demand of the electron tube can be further reduced.
  • the emitter and collector electrodes may comprise two-dimensional, mono- or multilayer materials, in particular graphene-like materials, like the gate electrode.
  • the at least one electrode layer of the gate electrode includes at least one of graphene, silicene, phosphorene, stanene, germanene, MoS 2 , C 3 N 4 and boron nitride.
  • graphene and the further preferred examples have a high electron transmission probability and heat conductivity (see e.g. [10]).
  • graphene has a transmission probability of 27 % for 66 eV electrons (see [5]).
  • the dopant of the at least one electrode layer comprises at least one of B, N, Bi, Sb, Au, NO 2 , ammonia and polyethyleneimine.
  • Preferred doping concentrations are e.g. 10 10 to 10 14 cm -2 .
  • the at least one electrode layer of the gate electrode is made of a material, which is insensitive to ionizing radiation.
  • this feature increases a long-term stability of the electron tube device operation, in particular under the effect of ionizing radiation.
  • This advantage is important in particular for applications of the invention in space crafts.
  • two-dimensional membranes of the above materials are stable under the effect of ionizing radiation. This stability can even be improved if the at least one electrode layer is made of an isotope selected for a higher insensitivity compared with other isotopes.
  • the at least one electrode layer can consist of graphene, which is completely made of C 12 isotopes.
  • the at least one electrode layer of the gate electrode is connected with a frame.
  • the frame is arranged between the electron emitter and the electron collector.
  • the at least one electrode layer is spanned on the frame, so that a stable mechanical support of the at least one electrode layer is provided.
  • the frame is electrically isolated with respect to the electron emitter and/or the electron collector, e.g. with ceramic spacers.
  • the spacers comprise aluminium oxide (sapphire, Al 2 O 3 ) or yttrium-stabilized zirconoxide (ZrO 2 ).
  • the gate electrode further comprises a supporting layer, which is connected with the at least one electrode layer.
  • the supporting layer carries the at least one electrode layer.
  • this increases the mechanical stability of the gate electrode and the positioning of the gate electrode with a distance relative to both of the electron collector and the electron emitter.
  • the supporting layer has a thickness in a range of 5 ⁇ m to 100 ⁇ m.
  • the supporting layer is made of silicon, which has advantages in terms of mechanical stability and heat conductivity.
  • the supporting layer is made of germanium or tungsten.
  • the supporting layer is a grid with supporting layer through-holes having diameters in a range of e. g. 1 ⁇ m to 100 ⁇ m.
  • the gate electrode may comprise multiple membrane-shaped electrically conductive or semiconductive electrode layers spaced from each other.
  • the gate electrode may include a stack of two-dimensional materials, preferably monolayers, each providing an electrode layer.
  • the material thickness and through-holes of the electrode layers are selected such that the gate electrode has an electron transparency of at least 20 %, preferably at least 25 %, particularly preferred 50 % or more.
  • multiple electrode layers can be manufactured by a growing process, wherein the electrode layers are deposited with sacrificial layers there between, which are removed subsequently. This allows the adjustment of distances of the electrode layers below 0.1 ⁇ m, in particular below 10 ⁇ m.
  • Preferred examples of materials, which can be used for creating the sacrificial layers comprise Cu, Fe, Al, or oxides, like CaMnO 3 , SrMnO 3 , La 2 CuO 4 or YBa 2 C 3 O 7 , which can be etched with weak acids, or even frozen water, which can be removed after deposition of the electrode layers.
  • the application of the invention is not restricted to the three electrode embodiment with one electrode emitter, one gate electrode, having one or more electrode layers and being connected with one gate voltage source, and one electrode collector. It is alternatively possible to provide more electrodes, in particular to provide more gate electrodes, each being connected with a specific gate voltage source and including one or more electrode layers.
  • the electrode layer of the second and each further gate electrode may comprise a continuous layer or a layer having through-holes as described above.
  • the provision of multiple gate electrodes may provide advantages in terms of enhancing the possible spacing between the emitter and collector and reducing heat losses.
  • the structure of the electron tube device can be adapted to the particular application thereof.
  • the electrodes of the electron tube device are arranged within an evacuated container.
  • the electrodes can be arranged in a container, which includes a working gas.
  • the working gas like e.g. Cs vapor, Cs-O vapor or ionized Cs-vapor, is capable of reducing space charges in the gap between the electron emitter and the electron collector and/or influencing a work function of the electron emitter, the electron collector and/or the gate electrode.
  • Further examples of working gases are gases based on other alkali metals, like Rb or K, or Ba, optionally mixed with oxygen.
  • an electron tube device having one single electron emitter, one single electron collector and one or two gate electrodes.
  • the electron tube device can have multiple gate electrodes and/or multiple pairs of electron emitters and collectors, each with a gap accommodating one or more gate electrode(s).
  • the electron tube can include further components as it is known from conventional electron tubes. It is emphasized that the drawings are schematic illustrations only, which do not represent scaled versions of practical devices. With practical implementations of the invention, the skilled person will be able to select geometrical dimensions, structural properties, materials and the electric circuitry in dependency on the particular application requirements.
  • the electron tube device 100 for the vacuum tube application of the invention comprises an electron emitter 10, an electron collector 20 and a gate electrode 30.
  • the electron emitter 10 comprises a straight electrode filament (or planar plate) 11, which is made of e. g. of a metal refractory metal, e. g. tungsten, in particular coated, doped or impregnated with a work-function-reducing material, e.g. Ba, BaO, La or LaO, and electrically connected with ground potential (earth potential).
  • the electrode filament 11 may be supported by mechanical components, like a carrier 14 (see Figure 2 ).
  • an electrode heater filament 13 is provided for indirect heating the electrode filament 11.
  • the electron emitter 10 could be directly heated and/or provided with nanotubes pointing towards the gap 1.
  • the electron collector 20 comprises a straight electrode filament (or planar plate) 21 as well, which is made of e. g. a metal or a refractory metal, e.g. tungsten, steel, copper, gold, silver, which can be coated or doped to enhance its properties like heat radiation absorption/reflection or work function, wherein an exposed surface 22 of the electron collector 20 is arranged with a distance D from an exposed surface 12 of the electron emitter 10.
  • the distance D (width of gap 1) is e. g. 100 ⁇ m.
  • the area of each of the exposed surfaces 12, 22 is selected in dependency on the particular application and operation parameters of the electron tube device. It is pointed out that the emitter and collector electrodes may be realized as thin films, foils, or membranes to reduce the weight and/or the material demand of the electron tube device 100.
  • the electron emitter 10, electron collector 20 and gate electrode 30 are accommodated in a vessel 60, which is evacuated or filled with a working gas.
  • the vessel 60 is made of e. g. glass or plastic material, including feedthrough sections for supply lines connected with the electrode components.
  • the shape and size of the vessel 60 are adapted to the shape and size of the electrodes.
  • the gate electrode 30 comprises at least one membrane-shaped electrode layer 31, having a planar, preferably two-dimensional shape and extending in the gap 1 parallel to the parallel planar exposed surfaces 12, 22 of the electron emitter 10 and the electron collector 20, respectively.
  • a distance between the electron emitter 10 and the gate electrode 30 is e. g. 10 ⁇ m.
  • the electrode layer 31 is e. g. a graphene mono- or multilayer having through-holes with a diameter of 400 ⁇ m covering e. g. 50 % or 70 % of the area of the electrode layer 31 facing to the electron emitter 10. It is supported by a frame 33 as shown in Figures 2 and 5 .
  • the application of the invention is not restricted to the use of graphene as the electrode layer material, but rather possible with the other material examples as cited above or even with further semi-transparent two-dimensional materials having electric conductivity or semi-conductivity.
  • Figure 1 schematically illustrates a gate heater unit 36, which is arranged for heating the gate electrode 30.
  • the gate heater unit 36 is provided in direct contact with the electrode layer 31, and it contains e. g. a resistor heating for annealing (tempering) the electrode layer 31.
  • a resistor heating for annealing titanium dioxide
  • the gate heater unit 36 is a switchable component, so that the annealing can be conducted on request or in dependency on predetermined operation conditions of the electron tube device 100.
  • Figure 2 further shows a support structure 50, including a base plate 51 and electron collector spacers 53.
  • the base plate 51 is made e.g. of Al 2 O 3 with a through-hole 54.
  • the electron emitter 10 is arranged for emitting electrons through the through-hole 54 to the electrode layer 31.
  • the electron collector spacers 53 have a thickness defining the distance between the graphene electrode layer 31 and the electron collector 20.
  • the electron collector spacers 53 are made of e. g. Al 2 O 3 .
  • the graphene electrode layer 31 is supported by the frame 33, which is arranged on an inner side of the base plate 51 facing towards the electron collector 20.
  • the frame 33 carries the electron collector spacers 53, and it is made of a metal, e. g.
  • the electron collector spacers 53 could be directly supported by the base plate 51, so that the distance between the graphene electrode layer 31 and the electron collector 20 would not be limited by the thickness of the electron collector spacers 53.
  • the graphene electrode layer 31 is arranged on the frame 33 in particular by one of the following procedures. Firstly, the graphene electrode layer 31 can be manufactured separately with a conventional method and subsequently transferred and fixed to the frame 33. Alternatively, the graphene electrode layer 31 can be grown on an auxiliary layer, which is connected with the frame 33 and subsequently removed. Furthermore, the graphene electrode layer 31 can be grown on a supporting layer 34 (see Figure 4 ).
  • the electrode layer 31 could be electrically connected as follows. Firstly, the electrode layer 31, e.g. a graphene layer, is connected with an upper surface of the frame 33, wherein the upper surface of the frame 33 is not completely covered by the electrode layer 31. An outer section of the upper surface remains exposed. Subsequently, a thin metallic layer, e.g. a Pt layer, is deposited on the frame 33. The deposition is obtained using e.g. a sputtering or other thin film deposition process. The metallic layer creates the electric contact with the electrode layer 31, and the electrode layer 31 is fixed on the frame 33 by the metallic layer. Finally, the metallic layer is connected with a gate voltage source 32.
  • a gate voltage source 32 e.g. a gate voltage source 32.
  • the electron tube device 100 is configured for a connection with voltage sources, including the gate voltage source 32 and a collector voltage source 23.
  • the gate voltage source 32 provides a gate voltage Vg to be applied to the gate electrode 30.
  • the collector voltage source 23 provides a collector voltage Va to be applied to the electron collector 30.
  • the voltages Vg, Va are positive or negative or alternating voltages selected in dependency on the application of the electron tube device 100.
  • the electron emitter 10 is heated with the electrode heater filament 13. Electrons are released from the exposed surface 12 of the electron emitter 10. The electrons are accelerated e. g. by an accelerating electric potential created with the collector voltage source 23. Most of the electrons are transmitted through the electrode layer 31 of the gate electrode 30 to the electron collector 20. By the gate voltage Vg of the gate voltage source 32, the current to the electron collector 20 can be modulated. After passing the gate electrode 30, the energy of the electrons could be too low for reaching the collector electrode 20. This effect can be avoided by reducing the electric potential at the collector electrode 20, so that the electrons require less energy to reach the collector.
  • FIGs 3 and 4 illustrate a modified embodiment of the electron tube device 100 which has two gate electrodes 30, 30A, each of which being designed like the gate electrode 30 of Figures 1 and 2 .
  • the electron emitter 10, the electron collector 20 and the vessel 60 are provided as described with reference to Figures 1 and 2 .
  • the gate electrodes 30, 30A are supported on frames 33, 33A, so that the electrode layers 31, 31A have a mutual distance of e. g. 10 ⁇ m in the gap 1 between the electron emitter 10 and the electron collector 20.
  • Both frames 33, 33A are electrically isolated relative to each other, e.g. by an isolating layer 35 or by ceramic spacers.
  • the voltage sources include two gate voltage sources 32, 32A creating a potential at the gate electrodes 30, 30A relative to the electron emitter 10 and the electron collector 20, resp..
  • the support structure 50 includes a base plate 51 and a cover plate 52. Both plates 51, 52 are made e.g. of Al 2 O 3 with through-holes 54, 55, resp..
  • the electron emitter 10 and the electron collector 20 are arranged in the through-holes 54, 55, resp..
  • the graphene electrode layers 31, 31A of the gate electrodes 30, 30A are supported by the frames 33, 33A, which are arranged on inner sides of the base and cover plates 51, 52.
  • Figure 5 schematically shows a top view of the frame 33 having an outer shape, e.g. rectangular shape, which is adapted to the geometry of the support structure 50, and a through-hole with a shape, e.g. circular shape, which is adapted to the shape of the electron emitter 10.
  • the frame 33 has a double function in terms of positioning the electrode layer 31 relative to the electron emitter 10 (see Figures 2 , 4 ) and providing an electrical contact with the electrode layer 31.
  • the frame 33 is made of or at least covered with a conductive, e.g. metallic, or semi-conductive material, which is electrically coupled with the gate voltage source (see Figure 1 ).
  • the electrode layer 31 can be grown on a supporting layer 34.
  • a supporting layer is shown with an REM image in Figure 6 .
  • the supporting layer 34 is made of, e.g., Si with a hexagonal structure having a mesh diameter of some 10 ⁇ m, e. g. by anisotropic etching. It is noted that the provision of the supporting layer 34 is not strictly necessary. Due to the tear strength of two-dimensional materials, e.g. graphene, the electrode layer 31 can be created with an area of some cm 2 without an additional supporting layer. Those skilled in the art will appreciate that also stacks of several supporting layers with different hole diameters may be used advantageously.

Landscapes

  • Cold Cathode And The Manufacture (AREA)
EP14003487.7A 2014-10-10 2014-10-10 Dispositif de tube à électrons Withdrawn EP3007199A1 (fr)

Priority Applications (1)

Application Number Priority Date Filing Date Title
EP14003487.7A EP3007199A1 (fr) 2014-10-10 2014-10-10 Dispositif de tube à électrons

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
EP14003487.7A EP3007199A1 (fr) 2014-10-10 2014-10-10 Dispositif de tube à électrons

Publications (1)

Publication Number Publication Date
EP3007199A1 true EP3007199A1 (fr) 2016-04-13

Family

ID=51751867

Family Applications (1)

Application Number Title Priority Date Filing Date
EP14003487.7A Withdrawn EP3007199A1 (fr) 2014-10-10 2014-10-10 Dispositif de tube à électrons

Country Status (1)

Country Link
EP (1) EP3007199A1 (fr)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109003986A (zh) * 2018-08-07 2018-12-14 长江存储科技有限责任公司 存储器结构及其形成方法
CN110416244A (zh) * 2019-07-30 2019-11-05 云谷（固安）科技有限公司 显示面板及其制作方法
US10816828B2 (en) 2016-11-02 2020-10-27 Samsung Electronics Co., Ltd. Multi-stack graphene structure and device including the same
JP2021533546A (ja) * 2018-08-10 2021-12-02 ジョン ベネット 低電圧電子透過ペリクル

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20130169142A1 (en) * 2011-12-29 2013-07-04 Elwha Llc Electronic Device Graphene Grid
WO2014019594A1 (fr) 2012-07-30 2014-02-06 Max-Planck-Gesellschaft Zur Förderung Der Förderung Der Wissenschaften E.V. Dispositif et procédé destinés à une conversion d'énergie thermoélectronique

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20130169142A1 (en) * 2011-12-29 2013-07-04 Elwha Llc Electronic Device Graphene Grid
WO2014019594A1 (fr) 2012-07-30 2014-02-06 Max-Planck-Gesellschaft Zur Förderung Der Förderung Der Wissenschaften E.V. Dispositif et procédé destinés à une conversion d'énergie thermoélectronique

Non-Patent Citations (12)

* Cited by examiner, † Cited by third party
Title
A. BALANDIN; S. GHOSH; W. BAO; I. CALIZO; D. TEWELDEBRHAN; F. MIAO; C. N. LAU: "Superior Thermal Conductivity of Single-Layer Graphene", NANO LETTERS, vol. 8, 2008, pages 902
B. GUO; L. FANG; B. ZHANG; J. R. GONG: "Graphene Doping: A Review", INSCIENCES JOURNAL, vol. 1, no. 2, 2011, pages 80
BEIDOU GUO ET AL: "Graphene Doping: A Review", INSCIENCES JOURNAL, 27 April 2011 (2011-04-27), pages 80 - 89, XP055175178, DOI: 10.5640/insc.010280 *
C. LEE; X. WEI; J. KYSAR; J. HONE: "Measurement of the Elastic Properties and Intrinsic Strength of Monolayer Graphene", SCIENCE, vol. 321, 2008, pages 385
C. LI; M. T. COLE; W, LEI; K. QU; K. YING; Y. ZHANG; A. R. ROBERTSON; J. H. WARNER; S. DING; X. ZHANG: "Highly Electron Transparent Graphene for Field Emission Triode Gates", ADVANCED FUNCTIONAL MATERIALS, vol. 24, 2014, pages 1218
C. STEPHANOS: "Thermoelectronic Power Generation from Solar Radiation and Heat", DOCTORAL THESIS, 2012
H. LIU; Y. LIU; D. ZHU: "Chemical doping of graphene", JOURNAL OF MATERIALS CHEMISTRY, vol. 21, 2011, pages 3253
HONGTAO LIU ET AL: "Chemical doping of graphene", JOURNAL OF MATERIALS CHEMISTRY, vol. 21, no. 10, 1 January 2011 (2011-01-01), pages 3335 - 3345, XP055175186, ISSN: 0959-9428, DOI: 10.1039/C0JM02922J *
J. SCHWEDE; I. BARGATIN; D. C. RILEY; B. E. HARDIN; S. J. ROSENTHAL; Y. SUN; F. SCHMITT; P. PIANETTA; R. T. HOWE; Z.-X. SHEN: "Photon-enhanced thermionic emission for solar concentrator systems", NATURE MATERIALS, vol. 9, 2010, pages 762
J.-N. LONGCHAMP; T. LATYCHEVSKAIA; C. ESCHER; H.-W. FINK: "Low-energy electron transmission imaging of clusters on free-standing graphene", APPLIED PHYSICS LETTERS, vol. 101, 2012, pages 113117
S. MEIR: "Highly-Efficient Thermoelectronic Conversion of Heat and Solar Radiation to Electric Power", DOCTORAL THESIS, 2012
S. MEIR; C. STEPHANOS; T. H. GEBALLE; J. MANNHART: "Highly-efficient thermoelectronic conversion of solar energy and heat into electric power", JOURNAL OF RENEWABLE AND SUSTAINABLE ENERGY, vol. 5, 2013, pages 043127

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10816828B2 (en) 2016-11-02 2020-10-27 Samsung Electronics Co., Ltd. Multi-stack graphene structure and device including the same
US11067836B2 (en) 2016-11-02 2021-07-20 Samsung Electronics Co., Ltd. Multi-stack graphene structure and device including the same
CN109003986A (zh) * 2018-08-07 2018-12-14 长江存储科技有限责任公司 存储器结构及其形成方法
JP2021533546A (ja) * 2018-08-10 2021-12-02 ジョン ベネット 低電圧電子透過ペリクル
CN110416244A (zh) * 2019-07-30 2019-11-05 云谷（固安）科技有限公司 显示面板及其制作方法

Similar Documents

Publication Publication Date Title
Go et al. Thermionic energy conversion in the twenty-first century: advances and opportunities for space and terrestrial applications
Liang et al. Electron thermionic emission from graphene and a thermionic energy converter
Palnitkar et al. Remarkably low turn-on field emission in undoped, nitrogen-doped, and boron-doped graphene
EP2880676B1 (fr) Dispositif et procédé destinés à une conversion d'énergie thermoélectronique
RU2675791C2 (ru) Рентгеновское устройство
Yuan et al. Back-gated graphene anode for more efficient thermionic energy converters
EP2801102B1 (fr) Anode dotée d'une grille de suppresseur
CN107248489B (zh) 一种表面隧穿微型电子源及其阵列和实现方法
James et al. A review of surface functionalisation of diamond for thermionic emission applications
EP3007199A1 (fr) Dispositif de tube à électrons
JP5762411B2 (ja) 集束電界放出のためのカーボンナノチューブ配列
US20130313980A1 (en) Embodiments of a field emission device
US6806629B2 (en) Amorphous diamond materials and associated methods for the use and manufacture thereof
Hong et al. Fabrication of a compact glass-sealed x-ray tube with carbon nanotube cold cathode for high-resolution imaging
Jarvis et al. Uniformity conditioning of diamond field emitter arrays
JP7272641B2 (ja) 電子放出素子及び電子顕微鏡
CN109473326A (zh) 场发射电子源及其用途与真空电子器件及装置
US9627168B2 (en) Field emission device with nanotube or nanowire grid
EP3007202B1 (fr) Dispositif et procédé de conversion d'énergie thermoélectronique
Iacobucci et al. Angular distribution of field emitted electrons from vertically aligned carbon nanotube arrays
Bocharov et al. Operational characteristics of a graphene-based electron field emitter
Iacobucci et al. Carbon nanotube—Based cold cathodes: Field emission angular properties and temporal stability
Fratini et al. Carbon-nanotubes field emitter to be used in advanced X-ray source
Serbun et al. High field emission current density from structured CNT bundle cathodes
Dyuzhev et al. Vacuum Nanoelectronics Based on Semiconductor Field-Emission Structures: Current State and Development Prospects. Review

Legal Events

Date Code Title Description
PUAI Public reference made under article 153(3) epc to a published international application that has entered the european phase

Free format text: ORIGINAL CODE: 0009012

AK Designated contracting states

Kind code of ref document: A1

Designated state(s): AL AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HR HU IE IS IT LI LT LU LV MC MK MT NL NO PL PT RO RS SE SI SK SM TR

AX Request for extension of the european patent

Extension state: BA ME

STAA Information on the status of an ep patent application or granted ep patent

Free format text: STATUS: THE APPLICATION HAS BEEN PUBLISHED

STAA Information on the status of an ep patent application or granted ep patent

Free format text: STATUS: THE APPLICATION IS DEEMED TO BE WITHDRAWN

18D Application deemed to be withdrawn

Effective date: 20161014