US2927243A - Electron discharge device for signal translation - Google Patents

Description

March 1, 1960 c. c. cu'TLER 2,927,243

ELECTRON DISCHARGE DEVICE FOR SIGNAL TRANSLATION Filed Jan. 23. 1956 3 Sheets-Sheet 1 /Nl/ENTOR C. C. CUTLER A TTORNE V March l, 1960 c. c. CUTLER 2,927,243

ELECTRON DISCHARGE DEVICE FOR SIGNAL TRANSLATION Filed Jan. 23. 195e s sheets-sheet 2 /N VEA/ T OR c. c. cUrLE/P www ATTORNEY March 1, 1960 c. c. cuTLER ELECTRON DISCHARGE DEVICE FOR SIGNAL TRANSLATION Filed Jan. 23. 1956 3 Sheets-Sheet 3 V75 F/G. 7A

- Tron/Vey United States Patent ELECTRON DiSCI-ARGE BEVICE FOR SIGNAL TRANSLATION Cassius C. Cutler, Gillette, NJ., assigner to BellnTfele phone Laboratories, Incorporated, New York, NY., a corporation of New York Application January 2s, 1956, serial No. 560,547 Y tz claims. (c1. 315.30)

The present invention relates to an electron discharge device useful for obtaining electrical signal translation.'

downstream Vis used to signify proximity to ythe collector. Subordinate features of thepresent invention are novel "transducers for modulating an annular or'Y ribbon beam in the manner described and novel transducers forex- A principal object of the present inven-tion is to achieve in a. single device satisfactory signal translation over both high and low frequencies.

A related object is to 4achieve high gain over awide range of frequencies in a single device.

To these ends, the present invention employs a ,novelY technique fo'r achieving amplification. The technique in- Volves projecting an annular or ribbon electron'beam which has a thickness which is small compared to its circumference or width into a magnetic eld for flow along an extended path in the direction of the flux'lines of the eld and modulating this beam periodically along its circumference or width by an input transducer in accordance with variations in an applied signal. In particular, the input transducer functions sotliat periodically along the circumference orwidth of lthe beam, different electrons are modulated to a diiferentextent Vin accordance with applied signals. Such modulation-takes the form of deflection initially either in a direction parallel to the circumference or width dimension or in a direction parallel to the thickness dimension. However, because of both space charge effects land the presence of the magnetic eld, all such deectionseventually give rise to a spiral rotation of the affected electrons. The net effect is that the beam tends to develop into a series of spiral nebulae; there is a tendency to degeneration of the beam into discrete portions having different rotation characteristics in accordance with the applied signal. Moreover, it is found'that the amplitude-ofl the disturbances on the beam increases with travel in the longitudinal magnetic field and that such increase is exponential along the beam length. Accordingly, an amplified output signal may be extracted from the beam by asuitable output transducer responsive to the disturbance on the beam.

Such operation is clearly to be distinguished from thatfamiliar in beam-deection tubes where the whole beam is deflected transversely a uniform amount inraccordance with variations in an applied signal.

The principal feature of the present invention is -acombination for use in amplification which includes means for projecting an annular or ribbon electron beam in the direction of a magnetic field, an input Ytransducer for modulating the beam along its circumference or width'in accordance with an applied signal, Vand an outputftransducer responsive to the resultant disturbances on the beam, the output transducer being spaced from the vinput transducer downstream along the path of'ow a sufcient distance to permit the initial modulation to increase, whereby the output signal extracted `is an amplified replica of the signal applied to the input transducer. Moreover, the input transducer is characterized in that it converts signals applied thereto to a relative displacement of different electrons along the beam circumference or width. As herein usedpthe term upstream is used tosignify proximity to the electron sourcerwhereasl'theterm tracting'an output signal from the resulting disturbances f on an electron beam. Y Y AIn oneamplier embodiment of the invention, an annu- 'lar beam is projectedinto'a longitudinal'magnetic ield for travel parallel tothe ux `lines thereof. An inputv transducer 'is positioned adjacent lthe upstream end of the beamrand include-s a series of deflection plates arranged symmetrically around: the periphery of 'the'annu- Vlar beam for applying in accordance with sign-al information detlections'tothe beam which are periodic in a circumferential direction and which give rise to ysignal modulation of the vbeam. An output transducer is positioned adjacent the downstream end of the beam forV extracting an amplified signal from the modulations on thevbe'am andincludes a like series of pairs of plates spaced sym- 20 j of Veach pair being within the'quies'cent position ofthe metrically around theperiphery of the beam, one plate beamand the other Without.

lIn a second amplifier embodiment, a ribbon beam is projected for travel parallel tothe flux lines of alongi- "tudinal magnetic eld, andinputl and output Vtransducers areV positioned adjacent themupstrearn and downstream ends o'fthebeam, respectively. The input transducer in this caseadvantageousl-y is a biilar helix which comlprisestwo equi-pitch helical conductors interwoundalong a common axis. V"A filamentary cathode is positioned along-'such-common axis and elec'ztrons` emittedtherefrom are formed into a ribbon beam which passes through the biiilar helix, being modulated in a direction along its Y'width Vby alsignal applied between Ythe two conductors of the helix. The beam continues through a magnetic lfield space where the modulations grow and then passes an output transducer which extracts the output signal The output transducer kin this caseadvantageouslyl is a conductive sheet which 'is -positioned to interceptthefbeamandhas a series of aperturestherethrough.

YVarious 'other illustrative embodiments will also be described. n

Thefinvention will 'be better understood from the following more detailed description taken in conjunction with the accompanying drawings ,in which:

Fig. lA is a longitudinal-sectional kview ofan ampli-A iierembodiment of the present invention; Y Y

Figs. -lB and l1C are cross-sectional views of the `;am-

plier of Fig. l taken through lines B-B and C.-"-C,1rev

spectively; Y Figs. 2A, 3A, 4A, 5A, and'A are longitudinal-sectional' views, each showing the upstream portion of a tube of the general type shown in Fig. l but incorporating a ,i I

different form of input transducer;

Figs. 2B, 3B, 4B, 4C, 5B and6B show of the various Vtubes shown'in Figs. 2A through 6A;

Fig. y7A isr a longitudinal-sectional View of a portion of a tube'which is of the general type shown in Fig. l but which employs a plurality of pencil vbeams arranged rin a` circular array to vform in effect an'v annular beam Each of Figs. 9, l0 and 11 showsan alternative form Y of an output transducer; and

Fig. 12 shows in cut-away perspective an embodiment of the invention employingra ribbon beam.

ln.'general, there has been employed'a minimum of sectional viewsr at the upstream and downstream ends of the beam path.

The gun includes a heater 15, an annular cathode 16, a beam forming electrode 17 having an aperture aligned with the emissive portion of the cathode surface, and an accelerating anode comprising the outer plate 18 and the inner cylinder 19 which between them form an aperture aligned with the emissive surface for passage tlierepast of the electron beam 20. The input transducer comprises a circular array of dellection plates 22 disposed symmetrically around the cylinder 19. The input transducer serves to apply deflection forces periodically about the beams circumference as shown more clearly in Fig. 1B. It is characteristic that the spacing of the deection forces is such that the space period of the deecton forces or the wavelength of the deecting field along the beams circumference be small compared to the wavelength of the signal to be amplified. The deflection forces give rise to disturbances on the beam whose amplitudes increase exponentially along the length of the beam because of the combined eiect of space charge forces and the magnetic field. As is shown in Fig. 1B, input signals are applied from source 26 to the input winding of transformer 27. Each terminal of the secondary winding of the transformer is connected to a different set of alternate plates of the array 22 and the center tap is connected to the inner cylinder 19. Output transducer 14 includes a like circular array of a pair of conductive plates 23 positioned for extracting output signals from the disturbances on the beam. As is shown in Fig. 1C, the plates 23 are disposed to form inner and outer circular 4arrays of plates and each set of alternate plates of the inner array is interconnected with a set of alternate plates of the outer array and an output terminal 2S. A collector 24 is positioned beyond the plates 23 and serves to collect any current which passes through the plates.

Support members for the various elements of the tube have been omitted in the drawing for simplicity. Moreover, there is also omitted the lead-in conductors from suitable voltage sources required for maintaining appropriate potentials on the various tube elements. In operation, the cathode is biased to a potential slightly positive with respect to the beam focusing electrode and appreciably negative with respect to the accelerating anode and the various elements of the input transducer so that the beam will be projected toward the opposite end of the envelope, toward the output transducer and collector which also are biased positively with respect to the cathode.

Additionally, a solenoid 28 is provided surrounding envelope 11 for establishing a magnetic eld whose ux extends along the length of the beam path for providing forces on the beam suicient to focus the beam in the absence of signal modulations and for cooperating with the space charge forces on the beam for amplifying signal disturbances provided on the beam of the kind described.

In operation, during one half cycle of a signal applied by the input source, the potential of one set of alternate plates of the array 22 will be less than that of the inner cylinder 19 while the potential of the other set of alternate plates will be greater than that of cylinder 19. This results in a radial force on the electrons of the beam which varies inwardly and outwardly periodically around the circumference of the beam and serves to distort the beam which was initially annular to the shape shown in Fig. 1B. During the next half cycle, the potentials on alternate sets of plates are reversed, and the beam is aected accordingly. This disturbance is found thereafter to build up exponentially along the beam length in the presence of the magnetic eld. The plates 23 of the output transducer are disposed so that in the absence of modulation on the beamfthe beam will pass almost completely through the interspace between each pair of plates 23 and no appreciable output voltage will be set np across output terminals 2S.` However, ifpthe beam hasV been disturbed or modulated by application of an input signal, electrons will be intercepted by the plates 23 and an output voltage developedy across terminals 25. In particular, during the time corresponding to one-half of the applied signal cycle, the current will be intercepted by one half of the plates including one set of alternate outer plates and one set of alternate inner plates and during the time of the other half cycle by the other half of the plates including the other sets of alternate inner and alternate outer plates. Thus the signal modulations on the beam are converted into alternating current ow through any load connected across terminals 25.

It has also been found that the amount of transverse beam deection initiated by deection arrangement 13 is a function of the amount of current in the beam. For constant deection fields, an increase in beam current results in greater initial beam deflection, and, conversely, a decrease in beam current results in a smaller initial beam deection. This property may advantageously be employed to provide an alternative technique for modulating the electron beam, which, in fact, may be preferred for many applications. Such a technique is employed in the tube shown in Figs. 2A and 2B. Only the input section of this tube has been shown since the output transducer may be of the type shown in Fig. 1C.

The tube 210 shown in Figs. 2A and 2B includes an evacuated envelope, electron gun, and an input transducer 213. The electron gun is substantially of the same type as that of Fig. 1A but includes a control grid 214 which is associated with the beam forming electrode of the gun for greater control of the electron emission from the gun. The input transducer includes a deflection arrangement made up of a circular array of plates as that shown in Fig. 1B. However, in this case, the input signal is applied directly to the control grid to modulate the potential of the control grid and thereby vary the beam density, and the deection arrangement is used to set up electrostatic elds. To this end, one set of alternate plates of the array is kept at a xed potential greater than that on the inner cylinder of the deflection arrangement and the other set is kept at a fixed potential less than that `of the inner cylinder. This results in a constant distorting ield on the annular beam. However, the ex- 'tent of distortion of the beam shape is now increased or decreased as the current of the beam is correspondingly increased or decreased. Thus the disturbance of the beam will vary again in accordance with the applied signal. In the operation of this tube, the input transducer comprises both the deflection arrangement and the gun control grid. The modulations thereby produced on the beam may be extracted by a suitable output transducer, for example, of the kind shown in Fig. 1C.

Figs. 3A and 3B show a portion of a tube employing a third technique for modulating an annular beam in a manner characteristic of the principles of the invention. This technique utilizes an unbalance in the space charge forces in the beam to produce disturbances periodically around the circumference which, in turn, because of the magnetic fleld results in a distortion of the beam of the kind useful for signal amplification. Consider a uniform annular beam passing in equilibrium along the parallel flux lines of a magnetic eld. If the electron beam density is thereafter decreased over one small segment of the annular beam, the electrons in the beam at the boundaries of that segment experience unbalanced space charge forces directed generally toenana-1s 5 ward the lowe'r density segment. Such forces in the presence of a magnetic field result in the radial displacement of the boundary electrons which, in turn, creates additional space charge forces and thus additional displacements, etc., to effect an exponential buildup of the disturbance along the beam length. By providing, spaced around the circumference of the beam, several such segments of decreased current density, the disturbances initiated may be made to produce modulation on the beam of the type described with reference to Fig. 1B. Alternatively, by providing spaced around the circumference of the beam several segments of increased current density, the same effect can be achieved. In the tube shown in Figs. 3A and 3B, a variation of current density periodically around the circumference of the annular beam is achieved by a segmented control grid 215 positioned advantageously adjacent the electron source. This grid, as shown more clearly in Fig. 3B contains grid wires 216 over certain segmental portions of its annular aperture 217 and thus 'the current density of the beam in these segmental regions is affected by the voltage on the grid to a Vgreater degree than in the regions therebetween. In operation, source 26 serves to apply a signal voltage between-cathode 16 and control grid 2.15. As a result of the consequent variation in current density over the beam circumference,` modulations are produced on the beam resulting inbeam distortion o-f the same character as' described with reference to Fig. 1B. In this embodiment, the segmented grid serves as the input transducer. Thereafter, from the modulations thus produced an output VvoltageV may beam periodically around its circumference is provided be extracted downstream along the beam by a suitable 'f' output transducer, for example of the kind shown in Fig. 1C.

Figs. 4A, 4B and 4C show a modification of the tube of Figs. 3A and 3B employing as the input transducer two segmental grids 414 and 415 spaced apart along the annular beam. In the construction of this tube the grid portions of these control grids are out of alignment along the path of fiow, allowance beingmade for any spiral motion of the electrons so that any given segment of the annular beam will pass through the grid portion of one or the other of the two control grids but not both. Consequently, as the annular beam passes the grids, one set of alternate segmental portions is affected by the first grid `f1.4 and the other set of alternate segmental portions is affected by the second grid 415. Advantageously, a push-pull input signal arrangement of the kind shown in Fig. lB is then provided for applying the signal voltage to each grid in opposite phase with respect to the cathode. The net effect is that the beam is distorted by applied 'signals in the manner similar to that provided by the arrangement in Fig. 1B.

Figs. 5A and 5B and 6A and 6B show alternative ernbodirnents for establishing modulations of the kind desired on an annular beam by the use of defiection arrangements of the so-called distributed typewhich are of special utility at high frequencies. In the embodiment shown in Figs. 5A and 5B, `deflection of the beam vis provided by four helices 511 spaced around the beam symmetrically about conductive cylinder 512 positioned within the beam. In some instances, it may be desirable to vary the direction of the axes of the helices to make allowance for the circumferential component of beam velocity arising from the magnetic field so Lthat each helix interacts with the same group of electrons throughout its length. Although each helix is advantageously a plurality of signal wavelengths long, the spacing around the beam is such that the wavelength of the defiecting field around the circumference of the beam is less than the signal wavelength. Each helix advantageously is terminated to be substantially refiectionless. The signal to be amplified is supplied from a signal source and applied in-phase to the upstream end of each of the helices. Because of coupling between the wave on the by a single helix 611 and four conductive rods 612 are spaced symmetrically about its .periphery to provide a circumferential variation in the coupling between the beam and the wave traveling along the' helix. The signal to be amplied is applied between the helix and the conductive rods. By this arrangement also, there is provided distortion around the circumference of the beam in accordance with applied signals, and in the magnetic field because of space charge effects thisdisturbance will grow so that a suitable output.trans,ducer will be able to extract an amplified-replica ofthe signal.

Figs. 7A and 7B show aV modification of the tube vof Fig. l in which the modification' comprises the replacec, ment of a gun for producing a continuous annular `beam with a gun for providing -av plurality of pencil beams arranged in a circular array to form the equivalent of an annular beam. Electron gun 711 for forming the` pencil Vbeams is shown schematically as including a cathode which includes a plurality of emissive regions 712 spaced -in a circular array, VAdvantageously, each beam has associated with it its own focusing electrode. .Each of the pencil beams thus formed is projected through the interspace between one of the deection plates 713 and inner conductive cylinder 714 of an' input transducerwhich may be of the kind discussed hereinabove whereby itis deflected in accordance with -anapplied signal as previously described. Operation .of this tube is substantially the samecas that previously described. The plurality of pencil beams may be considered as forming a'composite annular beam initially having a nonuniform current density over Vits crosssection. The useof pencil beams does, however, have'particularadvantages in that it-facilitates construction ,of Aasuitable electron gun, and further it militates against yth'e'bearn breaking into lav'greater numberof periods than desired.

Before discussing output transducers -whichmaybe used in Vplace of the transducer of Fig. 1C for abstracting 'the signal modulation from the beam, it may be helpful to discuss in mo-re detail the nature of the`displacement of electrons of the beam as a result of signal modulationof vthe kind described. Fig. 8 is intended to illustrate the deflection paths of individual electrons of an annular beam in a longitudinal magnetic field when acted on by deflec tion forces periodic around its circumference. In particular, it is to be noted that the presence ofthe magnetic field results in a tangential component of velocity which adds to the radialv component of velocity resulting from the radial electric fields. Moreover, electrons 811 at a portion of the bean on which radially inward elds are acting are deflected in a direction substantially opposite to that of electrons S12 or electrons 813 at portions of the beam on which radially outward fields are acting. In particular,

electrons 811 and S12 move closer together whereas electrons 811 and 813 move farther apart, whereby density modulations occur aroundthe circumference. Moreover, there is a tendency for the bem to separate into spiraling segments as shown by the arrows when overload is reached. The space period of such modulations on thev beam can be controlled by controlling thespace period of the defiection fields applied to the beam, for example by-varying the number of deflection lplates in the transducer of Fig. l'B, or by varying-the number of helices in the'transducer of Fig.` 5, andfsuch` space periodl-is-independent of the frequency of the applied signal. This independence between the space period and the frequency of the applied signal is an important characteristic of such because the applied signal tends to produce longitudinal modulations on the beam in addition to the circumference modulations it produces with the transducers discussed herein. For the avoidance of intermodulation effects which would obscure the signal, it is important that the space period of the circumferential modulation be less, and preferably substantially less, for example one tenth, than the space period of the longitudinal modulations. Thus it is important that the spacing of deection elements around the circumference be such that oppositely directed deiiection elds set up by such elements be less than one half the wavelength of the applied signal.

Appreciation of the fact that as the result of signal modulation lthe beam has both radial and tangential deection components, each of which is a measure of the amplitude of the initial disturbance, facilitates an understanding of the requirements of a suitable output transducer.

The output transducer shown in Fig. 9 is one primarily responsive to the radial components of signal modulation. It comprises a first conductive plate 911 having an annular aperture 912 therethrough and a second conductive plate 913 positioned to intercept the electrons which pass through aperture 912. In one mode of operation, the beam is aligned to pass essentially completely through aperture 912 in the absence of any signal modulation. Then as a signal is applied to modulate the beam, the amount of beam current which continues through the aperture decreases in proportion to the extent of radial deection of the beam. Thus the amount of current reaching plate 913 varies in accordance with the level of the signal applied to modulate the beam (actually in accordance with the absolute value of the level of the applied signal since the beam current reaching plate 913 varies in the same manner for both the positive and negative swing of the applied signal). The current reaching plate 911 is also a measure of the signal.

In another mode of operation, a D.-C. bias is employed to establish a steady initial disturbance on the beam and :the beam thereafter is aligned such that only half the beam current will pass through the annular aperture. In this case, as a signal is applied, the modulation on the beam is decreased on the negative swing of the applied signal and increased on its positive swing so that the output current reaching conductor 913 will now vary linearly in accordance with the level of the signal applied to modulate the beam.

Fig. 10 shows an alternative output transducer responsive to both the radial and tangential components of signal modulation on the beam electrons for deriving an output signal therefrom. This transducer comprises a rst conductive plate 1011 having an annular aperture 1012 interrupted by radial segments 1013, and a second conductive plate 1014 positioned to intercept the electrons which pass through aperture 1012. The plates are aligned for maximum transmission past the plate 1011 in the absence of signal modulation on the beam. Signal modulation on the beam will thereafter vary the amount of current arriving at plate 1014 in accordance with such modulation.

Fig. 1l shows an alternative output transducer especially advantageous for use at high frequencies in deriving signal from the modulated beam. This transducer includes a rst conductive plate 1111 having a series of apertures therethrough in a circular array, a second conductive plate 1113 positioned to intercept beam current which passes .through such apertures, and a helical conductor 1114 positioned between the two plates and te-rminated at the upstream end in its characteristic impedance, and leading off to the load at its downstream end. The helical conductor serves to form a distributed type wave circuit. As previously explained, the amount of current passing through apertures 1112 may be made to' vary in accordance With the signal modulation on the beam. In this instance, the modulation on the beam is converted into density modulation in the current passing4 beyond the plate 1111. Such density modulation on the beam may be made to set up a traveling wave on the helical conductor if the longitudinal velocity of the beam is adjusted to match .the axial velocity of a wave induced in the helix in accordance with principles familiar in the traveling wave tube art. Por increased efficiency the variations in current arriving at the plate 1113, which is another measure of the output signal, may be used to augment the wave set up on the helix.

The discussion up to this point has been concerned primarily with devices which employ annular electron beams. However, the general principles set forth also are applicable to devices employing a ribbon beam having a thickness small compared to its width. lIn this case there is provided a detiection arrangement which deects the beam periodically along its width in accordance with an applied signal. To this end, it is feasible to employ deiiection arrays of the kind described with the simple modiiction of having Ithe defiecting elements positioned in a linear array along the beam width rather than in a circular array along the beam circumference. The output transducer similarly would be modied to be responsive to the signal modulation on such a Vribbon beam. The use of a ribbon beam also makes advantageous the use of an input transducer in which the deflection iields established by the applied signals tend in the absence of a magnetic eld to displace the electrons in a direction parallel to the wide dimension of the beam. In Fig. l2, there is shown schematically a tube of thiskind.

In the tube of Fig. 12, a ribbon beam is provided by the ilamentary cathode 150. Suitable means not shown of the kind familiar to a Worker in the art are associated with the cathode for forming the cathode emission into a ribbon beam and directing it in the longitudinal direction desired for iiow parallel to a magnetic iield provided by the permanent magnet 151 which surrounds the tube envelope. The input transducer comprises a bifilar helix 152 comprising a pair of equipitch interwound helices having a common axis and equal diameters. Advantageously, the fllamentary cathode is positioned along the common axis.

Input signals are applied by way of a balanced pair line to one end of the bilar helix so that corresponding points on contiguous turns of the two helices are substantially 180 degrees out of phase. The opposite end of the bifilar helix is advantageously made reflectionless. Excitation of this type provides at the region of exit of the ribbon beam from the surrounding biiilar helix an electric field which extends in the wide dimension of the beam and which alternates in direction with a space period therealong equal to the pitch of a single helical conductor.

Such a field provides forces, in accordance with signal modulation in the direction of the wide dimension of the beam, which reverse direction periodically therealong. It is important that the pitch of the bitilar helix (which is twice the pitch of each helical conductor) is small compared to the wavelength of the applied signal. Such forces tend to deflect electrons in the beam and the presence of the magnetic iield results in a displacement in the thickness dimension of the beam in a manner analogous to displacements previously described. Because of space charge effects, such displacements grow with beam travel in the magnetic eld.

Downstream along the path of travel, an output transducer is used to extract an amplilied output signal from the modulation on the beam. As shown, the output transducer comprises a conductive plate 155 which includes a series of apertures in a linear array and spaced apart a distance corresponding to the pitch of a single helix of the bilar helix of the input transducer. The

'holes are aligned with the position o'f 'the 'electron'beam in the absence of signal modulation and 'have -adiameter wider than the width of the electron beam in the absence of signal modulation. Beyond this plate is positioned a collector 156 which collects all current passing through the plate 155. Signal modulation of the beam will vary the amount of current reaching the collector in accordance with such modulation.

This arrangement is useful only'at frequenciesat which the total length of the bifilar helix of the input'transducer is small compared to the signal wavelength. At higher frequencies, it is advantageous-to interpose between the plate 155 and the collector i555r a distributed waveA circuit such as a single wire helix whose axis is alignedy with the apertures such that the current passing through such apertures sets up a traveling wave on the helix. In this case, one end of such helix is made'substantially reilectionless and the other end is coupled to utilization apparatus. In such an arrangement, Athe phase propagating characteristics of the output Vhelix should be matchedfto the phase propagating characteristics vof the input -bifilar helix and each is made a-pl-urality of wavelengths 'oft-he applied signal long. -f

Alternatively, it is feasible towsubstitute a biiilar helix of the kind used as the input transducer for the output transducer, terminating-one end to make it reflfectionless and abstracting the amplied wave from the other. in such an arrangement the apertured plate 155 and the collector are omitted and the spent electrons are collected by the bifilar helix.

It should be evident that the specific embodiments described are merely illustrative of the general principles involved. Various other arrangements may be devised by one skilled in the art without departing from the spirit and scope of the invention. In particular, it would be feasible in transducer arrangements of the kind shown in Fig. 1B to employ each plate as a separate channel advantageously in conjunction lwith a multipencil beam gun and apply a separate signal to each channel. The output transducer similarly would be adjusted to derive separate outputs from each pencil beam.

ln the succeeding claims, the term transverse dimension of the beam is used generically to mean both the width of a ribbon beam and the circumference of an annular beam.

What is claimed is:

l. ln combination, means for forming an electron beam for flow in a magnetic field along a substantially constant longitudinal path of flow, means upstream along the path of flow for modulating the beam periodically along its transverse dimension symmetrically with respect to said path in accordance with signal information with a space period less than the wavelength of the applied signal and creating signal disturbances on the beam which grow with beam travel in the magnetic field, and means downstream along the path of flow responsive to such signal disturbances for providing an output therefor.

2. In combination, means for forming an annular electron beam for flow in a magnetic field along a substantially constant longitudinal path of ow, means upstream along the path of flow for modulating the beam periodically along its circumference and symmetrically with respect to said path in accordance with signal information with a space period less than the wavelength of the applied signal and creating signal disturbances around the circumference of the beam which grow with beam travel in the magnetic field, and means downstream along the path of ow responsive to such signal disturbances for providing an output therefor.

3. In combination, means for forming a ribbon electron beam for flow in a magnetic field along a substantially constant longitudinal path of flow, means upstream along the path of flow for modulating the beam periodically along its width dimension and symmetrically with respect to said path in accordance with signal inforless-than' the' wavelength .of-the applied signal 'andfer'eating signal disturbances on rthe beam "which g'row with beam travel in the magnetic field, and means downstream along the path of flow responsive Vto such `vsignal disturbances for providing an output therefor.

4. In combination, meansY for forming an electron beam for flow in a magnetic field along a substantially constant ylongitudinal path, 'means upstream alorig the lpathof flow for modulating the beam periodicallyalong its transverse dimension and symmetrically with respect to said path in accordance withvsignal information including Va Vplurality of deflection means spaced v`apart along'the transverse-dimension ofthe beam with a s'pacing less than one-half the Wavelength of the applied-*sig- `nal lfor creating signal disturbances on the beam which Ngrow with beam travel in the magnetic field, andv means downstream along the path of flow responsive'to such signal 'disturbances for provid-ing "an Aoutput therefor.

5. In combination,I -means `for forming an annular beam for flow in a magnetic fieldlal'ong a substantially constant longitudinalpath vof How, an input transducer 4upstream along 'the path-'of flow comprising a plurality A means spaced periodically along the beams width for modulating the beam periodically along its width and symmetrically with respect to said path in accordance with signal information with a space period less than the wavelength of the applied signal for creating signal disturbances on the beam which grow with beam travel in the magnetic field, and an output transducer Adownstream along the path of ow responsive `to such signal disturbances.

7. In combination, means forming an annular electron beam for flow in a magnetic field along a substantially constant longitudinal path of llow, input mean-s upstream along the path of flow including a series of conductive means spaced apart around the circumference of the beam for simultaneously deilecting circumferentially spaced portions of the beam in different radial directions transverse to the path of llow in accordance with signal information for creating signal disturbances on the beam which grow with travel in the magnetic field,

and output means downstream along the path of flow responsive to the signal disturbances.

8. In combination, a bifilar helix adapted to be excited by signal information so that the potential corresponding points of contiguous turns of its two conductors is out-ofphase, a filamentary cathode positioned along the axis of the bilar helix for providing a ribbon beam for ow in a magnetic lield along a substantially constant path and for exit through said biiilar helix whereby the beam is modulated periodically along its Width and symmetrically with respect tot said path in accordance `with the signal information with a space period less than the wavelength of the applied signal, and output means along the path of iow responsive to the signal modulation on the beam.

9. In combination, means forming an electron beam for ow in a magnetic field along a substantially constant longitudinal path of ow, a plurality of means spaced apart along the transverse dimension of the beam and supplied with input information, alternate means being excited in phase and adjacent means out of phase,

,'Whereby'the beamis modulated periodically along its transverse dimension and summetrically with respect to lsaid path, and output means responsive to the beam cent plates being excited in opposite phase and alternate plates in phase whereby the beam is modulated periodically around its circumference and symmetrically with respect to said path in accordance with signal information, and output means downstream along the beam responsive to the modulation on the beam.

11. In combination, means forming an annular beam for flow in a magnetic eld along a substantially constant longitudinal path of ow, a plurality of helices spaced apart around the circumference of the beam each having its axis extend in the direction of the path of ow and having a characteristic axial velocity substantially equal to the beam velocity for modulating the beam periodically around its circumference and symmetrically with respect to said path in accordance with signal information with a space period less than the wavelength of the applied signal, and output means responsive to the signal modulation on the beam.

12. In combination, means forming an electron beam having a thickness dimension substantially less than its widest cross-sectional dimension for ow in a magnetic field along a substantially constant longitudinal path, means for producing a plurality of distinct transverse bunches of electrons in the beam, said means including a plurality of spaced means upstream along the path of ow for modulating said beam periodically along its transverse dimension in response to signal information, said last-mentioned means having a transverse space period with respect to said path less than the wavelength of the applied signal, and output means downstream along the path of ow responsive to the signal modulations on the beam.

References Cited in the le of this patent UNITED STATES PATENTS 2,064,469 Haeff Dec. 15, 1936 2,075,717 Hehlgans Mar. 30, 1937 2,103,645 Schlesinger Dec. 28, 1937 2,206,668 Hollmann July 2, 1940 2,420,846 Strutt et a1. May 20, 1947 2,602,145 Law July l, 1952 2,793,315 Haei et al. May 21, 1957 2,824,997 Haetf Feb. 25, 1958 2,828,439 Fletcher Mar. 25, 1958 cre sur' umwmur-

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