EP3489987A1 - Internal load for travelling-wave tube using a delay line in a folded waveguide - Google Patents
Internal load for travelling-wave tube using a delay line in a folded waveguide Download PDFInfo
- Publication number
- EP3489987A1 EP3489987A1 EP18205842.0A EP18205842A EP3489987A1 EP 3489987 A1 EP3489987 A1 EP 3489987A1 EP 18205842 A EP18205842 A EP 18205842A EP 3489987 A1 EP3489987 A1 EP 3489987A1
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- Prior art keywords
- guide
- folded
- slow wave
- plate
- central plate
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Classifications
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
- H01J23/16—Circuit elements, having distributed capacitance and inductance, structurally associated with the tube and interacting with the discharge
- H01J23/24—Slow-wave structures, e.g. delay systems
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
- H01J23/16—Circuit elements, having distributed capacitance and inductance, structurally associated with the tube and interacting with the discharge
- H01J23/24—Slow-wave structures, e.g. delay systems
- H01J23/26—Helical slow-wave structures; Adjustment therefor
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J23/00—Details of transit-time tubes of the types covered by group H01J25/00
- H01J23/16—Circuit elements, having distributed capacitance and inductance, structurally associated with the tube and interacting with the discharge
- H01J23/24—Slow-wave structures, e.g. delay systems
- H01J23/26—Helical slow-wave structures; Adjustment therefor
- H01J23/27—Helix-derived slow-wave structures
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J25/00—Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
- H01J25/02—Tubes with electron stream modulated in velocity or density in a modulator zone and thereafter giving up energy in an inducing zone, the zones being associated with one or more resonators
- H01J25/025—Tubes with electron stream modulated in velocity or density in a modulator zone and thereafter giving up energy in an inducing zone, the zones being associated with one or more resonators with an electron stream following a helical path
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J25/00—Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
- H01J25/34—Travelling-wave tubes; Tubes in which a travelling wave is simulated at spaced gaps
- H01J25/36—Tubes in which an electron stream interacts with a wave travelling along a delay line or equivalent sequence of impedance elements, and without magnet system producing an H-field crossing the E-field
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J25/00—Transit-time tubes, e.g. klystrons, travelling-wave tubes, magnetrons
- H01J25/34—Travelling-wave tubes; Tubes in which a travelling wave is simulated at spaced gaps
- H01J25/36—Tubes in which an electron stream interacts with a wave travelling along a delay line or equivalent sequence of impedance elements, and without magnet system producing an H-field crossing the E-field
- H01J25/38—Tubes in which an electron stream interacts with a wave travelling along a delay line or equivalent sequence of impedance elements, and without magnet system producing an H-field crossing the E-field the forward travelling wave being utilised
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J9/00—Apparatus or processes specially adapted for the manufacture, installation, removal, maintenance of electric discharge tubes, discharge lamps, or parts thereof; Recovery of material from discharge tubes or lamps
- H01J9/24—Manufacture or joining of vessels, leading-in conductors or bases
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P9/00—Delay lines of the waveguide type
- H01P9/006—Meander lines
Definitions
- the present invention relates to a folded slow wave guide or waveguide line for a traveling wave tube of the acronym TOP.
- the grouping of the electrons in a packet is obtained by placing the beam in the field of a progressive wave whose phase velocity is equal to the speed of the electrons.
- the electrons see the field of a standing wave. The electrons are slowed on one alternation and accelerated on the next.
- a bundle of electrons forms around the phase for which we move from an accelerator field to a decelerating field.
- a conventional waveguide of rectangular or cylindrical section is not suitable for interaction because the phase velocity of the wave propagating in this guide is greater than the speed of light while the velocity of the electrons is lower. at the speed of light.
- an electric field parallel to the displacement of the electrons is required, whereas the fundamental mode of rectilinear guides of rectangular or cylindrical section is perpendicular to the axis of the guide.
- a special guide called slow waveguide or delay line is required. Most often the delay line is a periodic line obtained by repetitively translating a basic cell, to obtain a succession of identical cells. This is the case of the propeller, the line with coupled cavities, the interdigital line ...
- a so-called folded-delay line is often used.
- This line is obtained by periodically positioning rectangular waveguide sections perpendicular to the beam axis, and alternatively connecting the straight guide sections by 180 ° E plane bends.
- the crooked view of the folded guide has the shape of a coil.
- the beam slip hole is located in the middle of the straight rectangular guide section.
- the electric field in the guide is perpendicular to the long side of the guide, and therefore parallel to the movement of electrons, which allows to modulate the beam.
- the electron then moves in the sliding hole, opens into the right guide section where it undergoes the action of the electric field (interaction space), crosses the slip hole and opens into the next interaction space .
- the electron thus sees the successive interaction spaces with a period equal to the pitch of the line whereas the geometric period of the line is equal to twice the pitch.
- the pitch is the distance between two straight guides separated by an elbow.
- the length of the folded waveguide (right part and bends) is determined so that the phase shift of the wave in the waveguide corresponds to the phase variation related to the displacement of electrons from one interaction space to the next.
- Traveling wave tubes use a delay line with a number of sections greater than or equal to 2.
- the input section is terminated by a load and the output section begins with a load.
- Intermediate sections begin and end with a load.
- a charge is defined as a volume containing an RF wave absorbing material connected to the delay line, such that, in the plane of the connection, the impedance presented by the volume is as close as possible to the characteristic impedance of the line to be delay in order to achieve good adaptation (i.e., minimize the wave reflected by the load).
- the figure 1 schematically represents a delay line or waveguide for traveling wave tube comprising three sections 1, 2, 3.
- the delay line shown comprises an input 4 and an output 5.
- the charges 6 at the exit of the first section 1, at the entry of the second section 2, at the exit of the second section 2, and at the entrance of the third section 3 are called charge at the cutoff or "sever loads" in the English language.
- the electron beam passes through a slip hole without an RF field, which helps to ungroup the beam (so it is a loss of modulation).
- the length of the different sections is determined so as to limit the gain, given the reflection coefficient of the loads at the cut.
- the most common TOPs use a delay line comprising a propeller 7 held in a sleeve 8 by three dielectric uprights 9.
- the charge is generally made by depositing on the uprights 9 supporting the helix 7 a layer of material having high microwave losses, such as graphite.
- a material with microwave losses is characterized by a finite electrical conductivity ⁇ (unlike a perfect conductor whose electrical conductivity is infinite), which results in a conduction current ⁇ E (E being the electric field) and losses resistive ⁇ E 2 .
- ⁇ E conduction current
- ⁇ E 2 the wave undergoes exponential attenuation as a function of distance.
- a load is produced whose attenuation (microwave loss) and the reflection coefficient increase progressively, thus making it possible to obtain good adaptation over a wide frequency band.
- the length of the charge leads to a significant loss of modulation, and therefore to a gain loss of the TOP, which must be compensated by an increase in the gain of the other sections, and therefore to an increase in the total length of the TOP.
- the figure 3 schematically represents the attenuation on an upright 9, as a function of the thickness z of the deposition of the material having high microwave losses, such as graphite.
- the periodic line in folded guide and the straight guide containing the load do not have the same impedance and it is necessary to make an adaptation between the two, which is not broadband, and limits the band of the TOP.
- This variant comprises a sudden transition between the periodic folded guide 10 and the microwave loss dielectric block 13 which is equivalent to charging the periodic folded guide 10 by a resonator with microwave losses having numerous resonances, which limits the frequency band in which the charge is well suited.
- An object of the invention is to overcome the problems mentioned above.
- Losses are progressively introduced into the folded guide line, which is analogous to the gradual increase in graphite deposition on the propeller supports.
- the material having microwave losses is a microwave loss dielectric.
- the wave undergoes an exponential attenuation with a maximum of power dissipated at the beginning of the attenuated zone if the distribution of the lossy material is uniform.
- At least one groove has a constant section and comprises an increasing amount of the same microwave loss dielectric when the abscissa increases along the axis of the guide oriented in the direction of wave propagation.
- At least one groove has a constant or increasing section when said abscissa increases and is full of microwave loss dielectric whose level of microwave losses increases as said abscissa increases.
- the microwave loss material is a layer of a mixture of metals selected from iron, nickel, molybdenum, and titanium, at least partially covering the inner surface of a groove.
- At least one groove has a section whose stop length is constant and comprises an increasing amount of a layer of the same said mixture of metals when said abscissa increases.
- At least one groove has a section whose stopping length is constant or increasing as said abscissa increases and comprises a layer of the same said mixture of metals.
- the method further comprises a step of closing the guide by the lower plate and the upper plate, respectively fixed on the lower face and on the upper face of the central plate.
- the present invention consists in progressively introducing electromagnetic losses into the folded guide delay line to avoid a sudden transition between the periodic line and a rectangular guide, or between the periodic line and a dielectric block. , equivalent to increasing the graphite deposition on the amounts of a propeller delay line known from the state of the art.
- the folded guide delay line is coupled to another transmission line which has significant losses, and the coupling between the two lines increases in the direction of propagation of the wave. If we define a cell as the volume delimited by two planes perpendicular to the axis of the beam distant by one step (that is to say the distance between two straight guides separated by an elbow), the amplitude of the wave decreases from one cell to the next.
- two grooves 25 of variable section increasing with the abscissa of the z-axis of the guide, in this case symmetrical with respect to the mean plane of the central plate 20, are formed on the inner face of the guide of the lower plate 23 and on the inner face of the guide of the upper plate 24, and are filled with lossy dielectric material microwaves, such as a ceramic material (alumina, beryllium oxide, aluminum nitride) sintered with elements adding microwave losses (carbon, iron, titanium, ).
- a ceramic material alumina, beryllium oxide, aluminum nitride
- the transmission line with high electromagnetic losses can be machined in the lower plates 23 and / or 24 which are brazed with the central plate 20 in which the coil 22 is machined to form the folded guide delay line. It is therefore a hollow waveguide machined in the lower plates 23 and / or higher 24. It can also be machined in part or completely in the central plate 20.
- the figure 9 is a sectional view of a folded waveguide for traveling wave tube according to one aspect of the invention.
- the figure 10 represents different section sections of the example of the figure 9 .
- any embodiment comprising at least one groove 25 of variable section (variable or constant), made along the longitudinal axis z of the guide, on at least one inner face to the guide of the lower plate, the upper plate or the central plate, comprising at least partially a material having microwave losses, is possible.
- the grooves 25 it is possible to fill all or part of the grooves 25 with one or more microwave loss dielectrics, or deposit on the walls one or more microwave loss materials, so that along said longitudinal axis oriented in the direction of propagation of the wave, when the abscissa increases, the amplitude of the wave is attenuated by 20 dB between the beginning and the end of the load.
- At least one groove 25 may have a constant section and include an increasing amount of the same microwave loss dielectric as said abscissa increases.
- At least one groove 25 may have a constant or increasing section as said abscissa increases and be full of microwave loss dielectric whose level of microwave losses increases as the abscissa increases.
- At least one groove 25 may have a section whose stop length is constant and comprise an increasing quantity of a layer of the same mixture of metals chosen from: iron, nickel, molybdenum, titanium, at least partially covering the inner surface of a groove as the abscissa increases.
- At least one groove 25 may have a section whose stop length is constant or increasing when said abscissa increases and comprise a layer of the same mixture of metals chosen from: iron, nickel, molybdenum, titanium.
- a low height of the loss guide may correspond to a guide operating below the cutoff frequency and therefore to energy that does not propagate in the loss guide. In this case the guide behaves rather like a damped resonant cavity coupled to the folded guide.
- Plates generally parallelepipedic can be made by conventional methods of rolling or milling.
- the beam slip hole 21 can be made by electroerosion, and the slot 22 in the central plate can be made by wire EDM.
- the grooves 25 can be made by micro-milling or electroerosion.
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- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Waveguides (AREA)
- Microwave Tubes (AREA)
- Constitution Of High-Frequency Heating (AREA)
Abstract
Ligne à onde lente en guide replié munie d'une charge interne comprenant :- une plaque centrale (20) comprenant un trou (21) de glissement de faisceau, rectiligne de même direction que l'axe longitudinal (z) de la plaque centrale (20), et une fente (22) repliée en forme de serpentin ayant ses replis dans le sens de la largeur du guide ;- une plaque inférieure (23) et une plaque supérieure (24) fermant le guide d'onde, respectivement disposées sur et sous la plaque centrale (20) ;- au moins une rainure (25) de section pouvant être variable, réalisée selon l'axe longitudinal (z) du guide, sur au moins une face interne au guide de la plaque inférieure (23), la plaque supérieure (24) ou la plaque centrale (20), comprenant au moins partiellement un matériau présentant des pertes hyperfréquences ;pour former un guide à onde lente fermé dans lequel se propage une onde lente hybride dont l'amplitude est atténuée d'au moins 20 dB entre le début et la fin de la partie de la ou les rainures contenant un matériau à pertes.Slow wave line in folded guide provided with an internal load comprising: - a central plate (20) comprising a beam sliding hole (21), rectilinear in the same direction as the longitudinal axis (z) of the central plate ( 20), and a serpentine-shaped slit (22) having its folds in the direction of the width of the guide: - a lower plate (23) and a top plate (24) closing the waveguide respectively disposed on and under the central plate (20) - at least one groove (25) of variable section, made along the longitudinal axis (z) of the guide, on at least one inner face of the guide of the lower plate (23) the upper plate (24) or the central plate (20), at least partially comprising a material having microwave losses, to form a closed slow wave guide in which a hybrid slow wave is propagated whose amplitude is attenuated by at least 20 dB between the beginning and the end of the part of the o u the grooves containing a lossy material.
Description
La présente invention concerne une ligne à retard ou guide à onde lente replié pour tube à ondes progressives d'acronyme TOP.The present invention relates to a folded slow wave guide or waveguide line for a traveling wave tube of the acronym TOP.
Dans la plupart des tubes hyperfréquence l'interaction entre l'onde et le faisceau est décomposée en deux étapes :
- une première étape : obtenir un groupement des électrons en paquets, c'est-à-dire réaliser une modulation de densité du courant du faisceau au rythme du signal hyperfréquence ; et
- une deuxième étape : placer les paquets d'électrons ainsi obtenus dans une phase où ils sont ralentis par le champ afin de céder leur énergie à l'onde.
- a first step: obtaining a grouping of the electrons in packets, that is to say carrying out a density modulation of the beam current at the rate of the microwave signal; and
- a second step: place the electron packets thus obtained in a phase where they are slowed down by the field in order to give up their energy to the wave.
Dans le cas des TOP, le groupement des électrons en paquet est obtenu en plaçant le faisceau dans le champ d'une onde progressive dont la vitesse de phase est égale à la vitesse des électrons. Dans un repère mobile les électrons voient le champ d'une onde stationnaire. Les électrons sont ralentis sur une alternance et accélérés sur la suivante. Un paquet d'électrons se forme autour de la phase pour laquelle on passe d'un champ accélérateur à un champ décélérateur.In the case of the TOPs, the grouping of the electrons in a packet is obtained by placing the beam in the field of a progressive wave whose phase velocity is equal to the speed of the electrons. In a moving frame the electrons see the field of a standing wave. The electrons are slowed on one alternation and accelerated on the next. A bundle of electrons forms around the phase for which we move from an accelerator field to a decelerating field.
Un guide d'onde classique, de section rectangulaire ou cylindrique ne convient pas pour l'interaction car la vitesse de phase de l'onde qui se propage dans ce guide est supérieure à la vitesse de la lumière alors que la vitesse des électrons est inférieure à la vitesse de la lumière. De plus il faut un champ électrique parallèle au déplacement des électrons alors que le mode fondamental des guides rectilignes de section rectangulaire ou cylindrique est perpendiculaire à l'axe du guide. Pour obtenir une vitesse de phase inférieure à celle de la lumière il faut un guide spécial appelé guide à ondes lentes ou ligne à retard. Le plus souvent la ligne à retard est une ligne périodique obtenue en translatant de façon répétitive une cellule de base, pour obtenir une succession de cellules identiques. C'est le cas de l'hélice, de la ligne à cavités couplées, de la ligne interdigitale ...A conventional waveguide of rectangular or cylindrical section is not suitable for interaction because the phase velocity of the wave propagating in this guide is greater than the speed of light while the velocity of the electrons is lower. at the speed of light. In addition, an electric field parallel to the displacement of the electrons is required, whereas the fundamental mode of rectilinear guides of rectangular or cylindrical section is perpendicular to the axis of the guide. In order to obtain a phase velocity lower than that of light, a special guide called slow waveguide or delay line is required. Most often the delay line is a periodic line obtained by repetitively translating a basic cell, to obtain a succession of identical cells. This is the case of the propeller, the line with coupled cavities, the interdigital line ...
Dans le domaine des TOP fonctionnant aux longueurs d'onde millimétriques on utilise souvent une ligne à retard dite en guide replié. Cette ligne est obtenue en positionnant de manière périodique des sections de guide d'onde rectangulaire perpendiculaires à l'axe du faisceau, et en reliant de manière alternative les sections de guide droit par des coudes plan E à 180°. La vue de travers du guide replié a la forme d'un serpentin. Le trou de glissement du faisceau est situé au milieu de la section droite de guide rectangulaire. Le champ électrique dans le guide est perpendiculaire au grand coté du guide, et donc parallèle au déplacement des électrons, ce qui permet de moduler le faisceau. L'électron se déplace donc dans le trou de glissement, débouche dans la section de guide droit où il subit l'action du champ électrique (espace d'interaction), retraverse le trou de glissement et débouche dans l'espace d'interaction suivant. L'électron voit donc les espaces d'interaction successifs avec une période égale au pas de la ligne alors que la période géométrique de la ligne est égale à deux fois le pas. Le pas correspond à la distance entre deux guides droits séparés par un coude.In the field of the TOPs operating at millimeter wavelengths, a so-called folded-delay line is often used. This line is obtained by periodically positioning rectangular waveguide sections perpendicular to the beam axis, and alternatively connecting the straight guide sections by 180 ° E plane bends. The crooked view of the folded guide has the shape of a coil. The beam slip hole is located in the middle of the straight rectangular guide section. The electric field in the guide is perpendicular to the long side of the guide, and therefore parallel to the movement of electrons, which allows to modulate the beam. The electron then moves in the sliding hole, opens into the right guide section where it undergoes the action of the electric field (interaction space), crosses the slip hole and opens into the next interaction space . The electron thus sees the successive interaction spaces with a period equal to the pitch of the line whereas the geometric period of the line is equal to twice the pitch. The pitch is the distance between two straight guides separated by an elbow.
La longueur du guide d'onde replié (partie droite et coudes) est déterminée pour que le déphasage de l'onde dans le guide corresponde à la variation de phase liée au déplacement des électrons d'un espace d'interaction au suivant.The length of the folded waveguide (right part and bends) is determined so that the phase shift of the wave in the waveguide corresponds to the phase variation related to the displacement of electrons from one interaction space to the next.
Les tubes à onde progressives utilisent une ligne à retard comportant un nombre de sections supérieur ou égal à 2. La section d'entrée est terminée par une charge et la section de sortie commence par une charge. Les sections intermédiaires commencent et se terminent par une charge. On appelle charge un volume contenant un matériau absorbant l'onde RF raccordé à la ligne à retard, tel que, dans le plan du raccord, l'impédance présentée par le volume soit la plus proche possible de l'impédance caractéristique de la ligne à retard afin de réaliser une bonne adaptation (c'est-à-dire minimiser l'onde réfléchie par la charge).Traveling wave tubes use a delay line with a number of sections greater than or equal to 2. The input section is terminated by a load and the output section begins with a load. Intermediate sections begin and end with a load. A charge is defined as a volume containing an RF wave absorbing material connected to the delay line, such that, in the plane of the connection, the impedance presented by the volume is as close as possible to the characteristic impedance of the line to be delay in order to achieve good adaptation (i.e., minimize the wave reflected by the load).
La
Les charges 6 en sortie de la première section 1, en entrée de la deuxième section 2, en sortie de la deuxième section 2, et en entrée de la troisième section 3 sont appelées charge à la coupure ou "sever loads" en langue anglaise. Entre la fin d'une ligne et le début de la suivante le faisceau d'électrons passe dans un trou de glissement sans champ RF, ce qui contribue à dégrouper le faisceau (c'est donc une perte de modulation).The
Si les coefficients de réflexion aux deux extrémités d'une section et le gain de la section sont trop élevés, il est possible d'observer une oscillation dans la section de ligne à retard. C'est pourquoi la longueur des différentes sections est déterminée de manière à limiter le gain, compte tenu du coefficient de réflexion des charges à la coupure.If the reflection coefficients at both ends of a section and the gain of the section are too high, it is possible to observe an oscillation in the delay line section. This is why the length of the different sections is determined so as to limit the gain, given the reflection coefficient of the loads at the cut.
Les TOP les plus répandus, dont un exemple est illustré sur la
Sur une ligne à retard de la
Dans une telle ligne à retard à hélice, la longueur de la charge conduit à une perte de modulation importante, donc à une perte de gain du TOP, qu'il faut compenser par une augmentation du gain des autres sections, donc à une augmentation de la longueur totale du TOP.In such a helix delay line, the length of the charge leads to a significant loss of modulation, and therefore to a gain loss of the TOP, which must be compensated by an increase in the gain of the other sections, and therefore to an increase in the total length of the TOP.
La
Dans le cas de TOP utilisant une ligne à retard en guide replié, il est connu d'interrompre les ondulations pour passer d'un guide replié 10 à un guide droit 11, dans lequel est placée une charge absorbant de l'énergie électromagnétique. Un tel guide droit peut être soit parallèle, comme représenté sur les
Pour de tels modes de réalisation, bien qu'utilisant une même section de guide, la ligne périodique en guide replié et le guide droit contenant la charge n'ont pas la même impédance et il est nécessaire de réaliser une adaptation entre les deux, qui n'est pas à large bande, et limite la bande du TOP.For such embodiments, although using the same guide section, the periodic line in folded guide and the straight guide containing the load do not have the same impedance and it is necessary to make an adaptation between the two, which is not broadband, and limits the band of the TOP.
En variante, comme représenté sur la
Cette variante comprend une transition brutale entre le guide replié périodique 10 et le bloc diélectrique 13 à pertes hyperfréquences qui équivaut à charger le guide replié périodique 10 par un résonateur à pertes hyperfréquences possédant de nombreuses résonances, ce qui limite la bande de fréquences dans laquelle la charge est bien adaptée.This variant comprises a sudden transition between the periodic folded
Un but de l'invention est de pallier les problèmes précédemment cités.An object of the invention is to overcome the problems mentioned above.
Il est proposé, selon un aspect de l'invention, une ligne à onde lente en guide replié munie d'une charge interne comprenant :
- une plaque centrale comprenant un trou de glissement de faisceau, rectiligne de même direction que l'axe longitudinal de la plaque centrale, et une fente repliée en forme de serpentin ayant ses replis dans le sens de la largeur du guide ;
- une plaque inférieure et une plaque supérieure fermant le guide d'onde, respectivement disposées sur et sous la plaque centrale ;
- au moins une rainure de section pouvant être variable, réalisée selon l'axe longitudinal du guide, sur au moins une face interne au guide de la plaque inférieure, la plaque supérieure ou la plaque centrale, comprenant au moins partiellement un matériau présentant des pertes hyperfréquences ;
- a central plate comprising a beam sliding hole, rectilinear in the same direction as the longitudinal axis of the central plate, and a folded slot in the form of a coil having its folds in the direction of the width of the guide;
- a bottom plate and an upper plate closing the waveguide respectively disposed on and under the central plate;
- at least one groove of variable section, made along the longitudinal axis of the guide, on at least one inner face of the guide of the lower plate, the upper plate or the central plate, comprising at least partially a material having microwave losses ;
Ainsi les réflexions de la charge sont minimisées, et l'atténuation de l'énergie électromagnétique n'est pas brutale.Thus the reflections of the charge are minimized, and the attenuation of the electromagnetic energy is not brutal.
On introduit progressivement les pertes dans la ligne en guide replié, ce qui présente une analogie avec l'augmentation progressive du dépôt de graphite sur les supports d'hélice.Losses are progressively introduced into the folded guide line, which is analogous to the gradual increase in graphite deposition on the propeller supports.
Dans un mode de réalisation, le matériau présentant des pertes hyperfréquences est un diélectrique à pertes hyperfréquences.In one embodiment, the material having microwave losses is a microwave loss dielectric.
Ainsi, l'onde subit une atténuation exponentielle avec un maximum de puissance dissipée au début de la zone atténuée si la répartition du matériau à pertes est uniforme.Thus, the wave undergoes an exponential attenuation with a maximum of power dissipated at the beginning of the attenuated zone if the distribution of the lossy material is uniform.
Selon un mode de réalisation, au moins une rainure a une section constante et comprend une quantité croissante d'un même diélectrique à pertes hyperfréquences lorsque l'abscisse augmente selon l'axe du guide orienté dans le sens de propagation d'onde.According to one embodiment, at least one groove has a constant section and comprises an increasing amount of the same microwave loss dielectric when the abscissa increases along the axis of the guide oriented in the direction of wave propagation.
Ainsi, une faible proportion de la puissance peut être absorbée au début de la charge et une proportion plus élevée ensuite, avec pour avantage de mieux répartir la puissance dissipée sur la longueur de la charge.Thus, a small proportion of the power can be absorbed at the beginning of the load and a higher proportion thereafter, with the advantage of better distributing the power dissipated over the length of the load.
Dans un mode de réalisation, au moins une rainure a une section constante ou croissante lorsque ladite abscisse augmente et est pleine de diélectrique à pertes hyperfréquences dont le niveau de pertes hyperfréquences augmente quand ladite abscisse augmente.In one embodiment, at least one groove has a constant or increasing section when said abscissa increases and is full of microwave loss dielectric whose level of microwave losses increases as said abscissa increases.
Ainsi, une faible proportion de la puissance peut être absorbée au début de la charge et une proportion plus élevée ensuite, avec pour avantage de mieux répartir la puissance dissipée sur la longueur de la charge.Thus, a small proportion of the power can be absorbed at the beginning of the load and a higher proportion thereafter, with the advantage of better distributing the power dissipated over the length of the load.
En variante, le matériau à pertes hyperfréquences est une couche d'un mélange de métaux choisis parmi fer, nickel, molybdène, et titane, recouvrant au moins partiellement la surface interne d'une rainure.Alternatively, the microwave loss material is a layer of a mixture of metals selected from iron, nickel, molybdenum, and titanium, at least partially covering the inner surface of a groove.
Ainsi, il n'est pas nécessaire d'usiner un bloc diélectrique, puis de braser ce bloc ou de le sertir dans les plaques inférieures ou supérieures afin d'assurer l'écoulement de la chaleur entre le bloc diélectrique où la puissance est dissipée et la source froide placée autour de la ligne à retard.Thus, it is not necessary to machine a dielectric block, then solder this block or crimp it in the lower or upper plates to ensure the flow of heat between the dielectric block where the power is dissipated and the cold source placed around the delay line.
Par exemple, au moins une rainure a une section dont la longueur d'arrête est constante et comprend une quantité croissante d'une couche de même dit mélange de métaux lorsque ladite abscisse augmente.For example, at least one groove has a section whose stop length is constant and comprises an increasing amount of a layer of the same said mixture of metals when said abscissa increases.
En variante, au moins une rainure a une section dont la longueur d'arrête est constante ou croissante lorsque ladite abscisse augmente et comprend une couche de même dit mélange de métaux.Alternatively, at least one groove has a section whose stopping length is constant or increasing as said abscissa increases and comprises a layer of the same said mixture of metals.
Il est également proposé, selon un autre aspect de l'invention, un procédé de fabrication d'une ligne à onde lente en guide replié munie d'une charge interne comprenant des étapes consistant à :
- percer dans une plaque centrale un trou de glissement de faisceau, rectiligne de même direction que l'axe longitudinal d'une plaque centrale, et une fente repliée en forme de serpentin ayant ses replis dans le sens de la largeur du guide ;
- réaliser au moins une rainure de section pouvant être variable, selon l'axe longitudinal du guide, sur au moins une face interne au guide d'une plaque inférieure, une plaque supérieure ou la plaque centrale, comprenant au moins partiellement un matériau présentant des pertes hyperfréquences ;
- disposer la plaque inférieure et la plaque supérieure fermant le guide d'onde, respectivement sous et sur la plaque centrale ;
- piercing in a central plate a beam sliding hole, rectilinear in the same direction as the longitudinal axis of a central plate, and a folded slot in the form of a coil having its folds in the direction of the width of the guide;
- performing at least one groove of variable section, along the longitudinal axis of the guide, on at least one internal face to the guide of a lower plate, an upper plate or the central plate, comprising at least partially a material having losses microwave;
- arranging the lower plate and the upper plate closing the waveguide, respectively under and on the central plate;
Dans un mode de mise en oeuvre, le procédé comprend, en outre, une étape consistant à fermer le guide par la plaque inférieure et la plaque supérieure, fixées respectivement sur la face inférieure et sur la face supérieure de la plaque centrale.In one embodiment, the method further comprises a step of closing the guide by the lower plate and the upper plate, respectively fixed on the lower face and on the upper face of the central plate.
L'invention sera mieux comprise à l'étude de quelques modes de réalisation décrits à titre d'exemples nullement limitatifs et illustrés par les dessins annexés sur lesquels :
- la
figure 1 illustre schématiquement une ligne à retard ou guide à onde lente pour tube à ondes progressives comprenant trois sections, selon l'état de la technique ; - la
figure 2 illustre schématiquement une ligne à retard comprenant une hélice maintenue dans un fourreau par trois montants diélectriques, selon l'état de la technique ; - la
figure 3 illustre schématiquement l'atténuation sur un montant d'une ligne à retard de lafigure 2 , en fonction de l'épaisseur du dépôt du matériau ayant des pertes hyperfréquences élevée, selon l'état de la technique ; - la
figure 4 illustre schématiquement une ligne à retard en guide replié, comprenant une charge absorbant de l'énergie électromagnétique dans un guide droit parallèle au trou de glissement du faisceau, selon l'état de la technique ; - la
figure 5 illustre schématiquement une ligne à retard en guide replié, comprenant une charge absorbant de l'énergie électromagnétique dans un guide droit parallèle au trou de glissement du faisceau et replié vers les cellules de la ligne , selon l'état de la technique ; - la
figure 6 illustre schématiquement une ligne à retard en guide replié, comprenant une charge absorbant de l'énergie électromagnétique dans un guide droit perpendiculaire au trou de glissement du faisceau, selon l'état de la technique ; - la
figure 7 illustre schématiquement une ligne à retard en guide replié interrompue par un bloc de diélectrique à pertes d'une géométrie déterminée pour minimiser les réflexions de la charge, selon l'état de la technique ; et - les
figures 8 ,9 et 10 illustrent schématiquement une vue d'ensemble et des vues en coupe d'un guide à onde lente replié pour tube à ondes progressives, selon un aspect de l'invention.
- the
figure 1 schematically illustrates a delay line or waveguide for traveling wave tube comprising three sections, according to the state of the art; - the
figure 2 schematically illustrates a delay line comprising a propeller held in a sleeve by three dielectric uprights, according to the state of the art; - the
figure 3 schematically illustrates the attenuation on an amount of a delay line of thefigure 2 as a function of the thickness of the deposition of the material having high microwave losses, according to the state of the art; - the
figure 4 schematically illustrates a folded guide delay line, comprising a charge absorbing electromagnetic energy in a straight guide parallel to the beam slip hole, according to the state of the art; - the
figure 5 schematically illustrates a folded guide delay line, comprising a load absorbing electromagnetic energy in a straight guide parallel to the beam slip hole and folded towards the cells of the line, according to the state of the art; - the
figure 6 schematically illustrates a folded guide delay line comprising a load absorbing electromagnetic energy in a straight guide perpendicular to the beam slip hole, according to the state of the art; - the
figure 7 schematically illustrates a folded-line delay line interrupted by a lossy dielectric block of a determined geometry to minimize reflections of the load, according to the state of the art; and - the
figures 8 ,9 and 10 schematically illustrate an overview and sectional views of a folded waveguide for traveling wave tube, according to one aspect of the invention.
Sur l'ensemble des figures, les éléments ayant des références identiques sont similaires.In all the figures, the elements having identical references are similar.
Dans la présente description, les modes de réalisation décrits sont nullement limitatifs, et les caractéristiques et fonctions bien connues de l'homme du métier ne sont pas décrites en détails.In the present description, the embodiments described are in no way limiting, and the characteristics and functions well known to those skilled in the art are not described in detail.
Sur la
une plaque centrale 20 comprenant un trou 21 de glissement de faisceau, rectiligne de même direction que l'axe longitudinal z de laplaque centrale 20, et une fente 22 repliée en forme de serpentin ayant ses replis dans le sens de la largeur du guide ;- une plaque inférieure 23 et une
plaque supérieure 24 fermant le guide d'onde, respectivement disposées sur et sous laplaque centrale 20 ; - au moins une rainure 25 de section pouvant être variable, réalisée selon l'axe longitudinal z du guide, sur au moins une face interne au guide de la
plaque inférieure 23, laplaque supérieure 24 ou laplaque centrale 20, comprenant au moins partiellement un matériau présentant des pertes hyperfréquences ;
- a
central plate 20 comprising abeam sliding hole 21, rectilinear in the same direction as the longitudinal axis z of thecentral plate 20, and aslot 22 folded serpentine having its folds in the direction of the width of the guide; - a
lower plate 23 and anupper plate 24 closing the waveguide respectively disposed on and below thecentral plate 20; - at least one
groove 25 of variable section, made along the longitudinal axis z of the guide, on at least one inner face of the guide of thelower plate 23, theupper plate 24 or thecentral plate 20, comprising at least partially a material with microwave losses;
En d'autres termes, la présente invention consiste à introduire de façon progressive des pertes électromagnétiques dans la ligne à retard en guide replié pour éviter une transition brutale entre la ligne périodique et un guide rectangulaire, ou entre la ligne périodique et un bloc de diélectrique, de manière équivalente à l'augmentation du dépôt de graphite sur les montants d'une ligne à retard à hélice connu de l'état de l'art.In other words, the present invention consists in progressively introducing electromagnetic losses into the folded guide delay line to avoid a sudden transition between the periodic line and a rectangular guide, or between the periodic line and a dielectric block. , equivalent to increasing the graphite deposition on the amounts of a propeller delay line known from the state of the art.
Pour ce faire la ligne à retard en guide replié est couplée à une autre ligne de transmission qui possède des pertes importantes, et le couplage entre les deux lignes augmente dans le sens de propagation de l'onde. Si l'on définit une cellule comme le volume délimité par deux plans perpendiculaires à l'axe du faisceau distant d'un pas (c'est-à-dire la distance entre deux guides droits séparés par un coude), l'amplitude de l'onde diminue d'une cellule à la suivante.To do this, the folded guide delay line is coupled to another transmission line which has significant losses, and the coupling between the two lines increases in the direction of propagation of the wave. If we define a cell as the volume delimited by two planes perpendicular to the axis of the beam distant by one step (that is to say the distance between two straight guides separated by an elbow), the amplitude of the wave decreases from one cell to the next.
Sur l'exemple de la
La ligne de transmission à fortes pertes électromagnétiques peut être usinée dans les plaques inférieure 23 et/ou supérieures 24 qui sont brasées avec la plaque centrale 20 dans laquelle est usiné le serpentin 22 afin de constituer la ligne à retard en guide replié. Il s'agit donc d'un guide d'onde usiné en creux dans les plaques inférieure 23 et/ou supérieures 24. Il peut également être usiné en partie ou totalement dans la plaque centrale 20.The transmission line with high electromagnetic losses can be machined in the
Sur l'exemple de la
La
La
En variante, tout mode de réalisation comprenant au moins une rainure 25 de section pouvant être variable (variable ou constante), réalisée selon l'axe longitudinal z du guide, sur au moins une face interne au guide de la plaque inférieure, la plaque supérieure ou la plaque centrale, comprenant au moins partiellement un matériau présentant des pertes hyperfréquences, est possible.Alternatively, any embodiment comprising at least one
Pour réaliser ces pertes électromagnétiques, il est possible de remplir en partie ou en totalité les rainures 25 avec un ou différents diélectriques à pertes hyperfréquences, ou déposer sur les parois un ou différents matériaux à pertes hyperfréquences, de sorte que selon ledit axe longitudinal orienté dans le sens de propagation de l'onde, lorsque l'abscisse augmente, l'amplitude de l'onde soit atténuée de 20 dB entre le début et la fin de la charge.To achieve these electromagnetic losses, it is possible to fill all or part of the
Les cas les plus explicites sont les suivants.The most explicit cases are as follows.
Au moins une rainure 25 peut avoir une section constante et comprendre une quantité croissante d'un même diélectrique à pertes hyperfréquences lorsque ladite abscisse augmente.At least one
En variante, au moins une rainure 25 peut avoir une section constante ou croissante lorsque ladite abscisse augmente et être pleine de diélectrique à pertes hyperfréquences dont le niveau de pertes hyperfréquences augmente quand l'abscisse augmente.Alternatively, at least one
En variante, au moins une rainure 25 peut avoir une section dont la longueur d'arrête est constante et comprendre une quantité croissante d'une couche de même mélange de métaux choisis parmi: fer, nickel, molybdène, titane, recouvrant au moins partiellement la surface interne d'une rainure lorsque l'abscisse augmente.In a variant, at least one
En variante, au moins une rainure 25 peut avoir une section dont la longueur d'arrête est constante ou croissante lorsque ladite abscisse augmente et comprendre une couche de même mélange de métaux choisis parmi: fer, nickel, molybdène, titane.In a variant, at least one
Le grand coté du guide usiné dans les plaques inférieures et supérieures détermine l'ouverture dans la ligne en guide replié, et donc le couplage entre les deux lignes de transmission. Une faible hauteur du guide à pertes peut correspondre à un guide fonctionnant en dessous de la fréquence de coupure et donc à une énergie ne se propageant pas dans le guide à pertes. Dans ce cas le guide se comporte plutôt comme une cavité résonante amortie couplée au guide replié.The large side of the guide machined in the lower and upper plates determines the opening in the line folded guide, and thus the coupling between the two transmission lines. A low height of the loss guide may correspond to a guide operating below the cutoff frequency and therefore to energy that does not propagate in the loss guide. In this case the guide behaves rather like a damped resonant cavity coupled to the folded guide.
Le procédé de fabrication d'une telle ligne à onde lente en guide replié munie d'une charge interne comprend des étapes consistant à :
- percer dans une plaque centrale (20) un trou (21) de glissement de faisceau, rectiligne de même direction que l'axe longitudinal (z) d'une plaque centrale (20), et une fente (22) repliée en forme de serpentin ayant ses replis dans le sens de la largeur du guide ;
- réaliser au moins une rainure (25) de section pouvant être variable, selon l'axe longitudinal (z) du guide, sur au moins une face interne au guide d'une plaque inférieure (23), d'une plaque supérieure (24) ou de la plaque centrale (20), comprenant au moins partiellement un matériau présentant des pertes hyperfréquences ;
- disposer la plaque inférieure (23) et la plaque supérieure (24) fermant le guide d'onde, respectivement sous et sur la plaque centrale (20) ;
- piercing in a central plate (20) a beam sliding hole (21) rectilinear in the same direction as the longitudinal axis (z) of a central plate (20), and a slit (22) folded into a coil shape having its folds in the direction of the width of the guide;
- producing at least one groove (25) of variable section, along the longitudinal axis (z) of the guide, on at least one inner face of the guide of a lower plate (23), an upper plate (24) or the central plate (20), at least partially comprising a material having microwave losses;
- arranging the lower plate (23) and the upper plate (24) closing the waveguide, respectively under and on the central plate (20);
Les plaques, généralement parallélépipédiques peuvent être réalisées par des procédés classiques de laminage ou fraisage.Plates, generally parallelepipedic can be made by conventional methods of rolling or milling.
Le trou 21 de glissement de faisceau peut être réalisé par électroérosion, et la fente 22 dans la plaque centrale peut être réalisée par électroérosion à fil.The
Les rainures 25 peuvent être réalisées par micro-fraisage ou par électroérosion.The
Claims (8)
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| FR1701253A FR3074364B1 (en) | 2017-11-28 | 2017-11-28 | INTERNAL LOAD FOR PROGRESSIVE WAVE TUBE USING A FADED DELAY LINE |
Publications (2)
| Publication Number | Publication Date |
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| EP3489987A1 true EP3489987A1 (en) | 2019-05-29 |
| EP3489987B1 EP3489987B1 (en) | 2020-09-16 |
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| EP18205842.0A Active EP3489987B1 (en) | 2017-11-28 | 2018-11-13 | Internal load for travelling-wave tube using a delay line in a folded waveguide |
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| US (1) | US10475617B2 (en) |
| EP (1) | EP3489987B1 (en) |
| JP (1) | JP7272778B2 (en) |
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| CA (1) | CA3025335C (en) |
| FR (1) | FR3074364B1 (en) |
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| DE112019000369B4 (en) * | 2018-03-07 | 2024-02-08 | Nec Network And Sensor Systems, Ltd. | Delay circuit, traveling wave tube and method for producing a traveling wave tube |
| CN110767971A (en) * | 2019-10-30 | 2020-02-07 | 中国电子科技集团公司第十二研究所 | Centralized attenuator and traveling wave tube comprising same |
| CN111017865B (en) * | 2019-11-27 | 2022-09-09 | 上海交通大学 | Preparation method for terahertz folded waveguide microstructure |
| CN111029231B (en) * | 2019-12-06 | 2021-09-07 | 中国电子科技集团公司第十二研究所 | Spiral line-based hybrid slow wave structure and design method thereof |
| US11422305B2 (en) * | 2020-12-02 | 2022-08-23 | Globalfoundries U.S. Inc. | Structures for filtering light polarization states on a photonics chip |
| CN112820610B (en) * | 2020-12-30 | 2024-08-02 | 中国电子科技集团公司第十二研究所 | Energy transmission coupling structure for band-shaped injection staggered grid traveling wave tube |
| CN114220723B (en) * | 2021-11-01 | 2024-10-18 | 中国电子科技集团公司第十二研究所 | Distributed attenuator and distributed attenuation method suitable for folded waveguide traveling wave tube |
| CN114783847B (en) * | 2022-03-29 | 2023-09-05 | 电子科技大学 | A novel slow-wave structure based on interleaved double grids and meandering waveguides |
| CN114710851A (en) * | 2022-04-01 | 2022-07-05 | 湖南理工职业技术学院 | A Design Method of Dielectric Total Reflector Applied to Single-Mode Metal Waveguide |
| CN114758938B (en) * | 2022-04-22 | 2025-08-08 | 中国工程物理研究院应用电子学研究所 | A weakly reflective folded waveguide slow-wave structure |
| CN114823252B (en) * | 2022-04-29 | 2023-07-14 | 电子科技大学 | A bidirectional multi-injection traveling wave cascade amplifier based on cold cathode |
| CN118962247B (en) * | 2024-08-07 | 2025-10-21 | 中国科学院空天信息创新研究院 | Method and device for determining electrical conductivity and inner surface roughness of folded waveguide |
Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4619041A (en) * | 1982-10-06 | 1986-10-28 | English Electric Valve Company Limited | Method for manufacturing coupled cavity travelling wave tubes |
| US5422596A (en) * | 1994-06-30 | 1995-06-06 | The United States Of America As Represented By The Secretary Of The Navy | High power, broadband folded waveguide gyrotron-traveling-wave-amplifier |
| US20120081003A1 (en) * | 2010-10-04 | 2012-04-05 | Samsung Electronics Co., Ltd. | Terahertz interaction circuit having ridged structure |
Family Cites Families (9)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3412279A (en) * | 1965-09-13 | 1968-11-19 | Varian Associates | Electromagnetic wave energy absorbing elements for use in high frequency electron discharge devices having traveling wave tube sections |
| US4158791A (en) * | 1977-02-10 | 1979-06-19 | Varian Associates, Inc. | Helix traveling wave tubes with resonant loss |
| JPS61284032A (en) * | 1985-06-07 | 1986-12-15 | Nec Corp | Cavity-coupled type traveling wave tube |
| US4695766A (en) * | 1986-08-01 | 1987-09-22 | Raytheon Company | Traveling wave tube and its method of construction |
| CN101673866A (en) * | 2009-07-22 | 2010-03-17 | 电子科技大学 | Curved channel waveguide slow-wave line |
| CN202352608U (en) * | 2011-10-11 | 2012-07-25 | 电子科技大学 | Tapered ridge loading serpentine waveguide slow-wave line |
| CN202855699U (en) * | 2012-10-25 | 2013-04-03 | 电子科技大学 | Zigzag waveguide slow-wave line |
| EP3392899B1 (en) * | 2015-12-18 | 2020-09-02 | Nec Network And Sensor Systems, Ltd. | Slow wave circuit and traveling wave tube |
| FR3069659B1 (en) * | 2017-07-27 | 2019-08-09 | Thales | SLOW WAVE GUIDE FOR PROGRESSIVE WAVE TUBE |
-
2017
- 2017-11-28 FR FR1701253A patent/FR3074364B1/en not_active Expired - Fee Related
-
2018
- 2018-10-25 JP JP2018200613A patent/JP7272778B2/en active Active
- 2018-11-13 EP EP18205842.0A patent/EP3489987B1/en active Active
- 2018-11-14 US US16/191,383 patent/US10475617B2/en active Active
- 2018-11-27 CA CA3025335A patent/CA3025335C/en active Active
- 2018-11-28 CN CN201811431228.0A patent/CN110021511B/en active Active
Patent Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4619041A (en) * | 1982-10-06 | 1986-10-28 | English Electric Valve Company Limited | Method for manufacturing coupled cavity travelling wave tubes |
| US5422596A (en) * | 1994-06-30 | 1995-06-06 | The United States Of America As Represented By The Secretary Of The Navy | High power, broadband folded waveguide gyrotron-traveling-wave-amplifier |
| US20120081003A1 (en) * | 2010-10-04 | 2012-04-05 | Samsung Electronics Co., Ltd. | Terahertz interaction circuit having ridged structure |
Non-Patent Citations (2)
| Title |
|---|
| KORY C ET AL: "Microfabricated W-Band Traveling Wave Tubes", INFRARED AND MILLIMETER WAVES AND 13TH INTERNATIONAL CONFERENCE ON TER AHERTZ ELECTRONICS, 2005. IRMMW-THZ 2005. THE JOINT 30TH INTERNATIONAL CONFERENCE ON WILLIAMSBURG, VA, USA 19-23 SEPT. 2005, PISCATAWAY, NJ, USA,IEEE, vol. 1, 19 September 2005 (2005-09-19), pages 85 - 86, XP010874888, ISBN: 978-0-7803-9348-6, DOI: 10.1109/ICIMW.2005.1572419 * |
| MINGLIANG LIAO ET AL: "A Rectangular Groove-Loaded Folded Waveguide for Millimeter-Wave Traveling-Wave Tubes", IEEE TRANSACTIONS ON PLASMA SCIENCE, IEEE SERVICE CENTER, PISCATAWAY, NJ, US, vol. 38, no. 7, 1 July 2010 (2010-07-01), pages 1574 - 1578, XP011310618, ISSN: 0093-3813 * |
Also Published As
| Publication number | Publication date |
|---|---|
| CN110021511B (en) | 2024-05-07 |
| CN110021511A (en) | 2019-07-16 |
| CA3025335C (en) | 2025-09-23 |
| EP3489987B1 (en) | 2020-09-16 |
| FR3074364A1 (en) | 2019-05-31 |
| US20190164714A1 (en) | 2019-05-30 |
| CA3025335A1 (en) | 2019-05-28 |
| FR3074364B1 (en) | 2019-10-25 |
| JP7272778B2 (en) | 2023-05-12 |
| JP2019102438A (en) | 2019-06-24 |
| US10475617B2 (en) | 2019-11-12 |
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