LOW NOISE MAGNETICALLY TUNED RESONANT CIRCUIT

Abstract: A magnetically tuned resonant circuit (10) includes a ferrimagnetic or gyromagnetic body (46) such as a YIG sphere which is disposed within a r.f. structure (30). The r.f. structure (30) is disposed between a pair of pole pieces (24,38) of a biasing magnet and flux return path (20). To reduce fluctuations in magnetic fields through the gyromagnetic body (46), the body (46) is isolated from conductive surfaces, or the bulk of conductive surfaces in the region adjacent to the magnetic body (46) are reduced. A break (131a,131b) may be provided in the electrical continuity around the r.f. structure (30). These features reduce the magnitude of thermally induced eddy current flow in conductive regions adjacent to the resonant body (46) and hence reduce random magnetic field variations which produce random variations in the frequency characteristics of the magnetically tuned resonant circuit (10).

Description: Background of the Invention This invention relates to a magnetically tuned resonant circuit comprising: a) means for producing magnetic flux; b) means for providing a magnetic flux path, having a pair of opposing spaced surfaces; c) a magnetically inert member comprising a magnetically inert body member and disposed between said pair of opposing spaced surfaces and having a pair of coaxial conductors each having an inner conductor and an outer conductor dielectrically spaced therefrom, with the outer conductor electrically connected to the magnetically inert member; and d) a gyromagnetic member disposed in an aperture in said inert body member, with said inert member disposed to have said magnetic flux directed through said gyromagnetic member, and the inner conductors of the said coaxial conductors coupled about the gyromagnetic member. As it is known in the art, magnetically tuned resonant circuits, such as YIG filters, are used in many radio frequency applications, such as radar receivers. One application for a magnetically tuned resonant circuit is in a radio frequency oscillator. In particular, one type of oscillator includes a YIG band pass filter disposed in the feedback circuit of an amplifier. When the open loop gain and phase conditions of the oscillator are satisfied simultaneously at a certain frequency, that is, when the open loop gain is greater than unity and the open loop phase shift is equal to an integer multiple of 2π radians, the circuit will operate as an oscillator at that particular frequency. A second application for a magnetically tuned resonant circuit is as a dispersive element in an interferometer type of frequency discriminator. For example, a microwave voltage controlled oscillator (VCO), which typically produces signals with high levels of frequency modulation (FM) noise, is stabilized with a frequency lock loop using the YIG filter as the dispersive element in the frequency discriminator. In "YIG resonators and systems", at pages 47 to 56, No. 684, December 1983, vol. 55, Electronic Engineering, J. Helszajn describes the use of single crystal Yttrium Iron Garnet (YIG) as a microwave resonator, based on the property that for a spherical YIG body, the resonance frequency is only related to the direct magnetic field and not to the dimensions of the structure. A YIG oscillator is depicted as having the sphere disposed in an airgap of a re-entrant electro-magnet. A YIG band-pass filter is described as consisting of a YIG resonator at the intersection of two orthogonal microwave transmission lines, which may be wire loops or semi-loops, striplines, or waveguides. Semi-loops are placed on either side of the resonator to minimise direct coupling between the orthogonal circuits. Circuits which are shown utilizing a YIG resonator are a YIG Gunn oscillator circuit, a FET YIG oscillator, an amplitude type tunable YIG discriminator, and a linearisation circuit. It is further stated that eddy currents may be minimised by increasing the resistivity of the current paths by using high resistivity steels for the YIG housing and by using steel laminations or ferrite polycrystalline materials for the core of the electromagnet, and that the induced eddy current in the YIG housing are sometimes minimised by fabricating it from a suitable plastic material and plating the microwave surfaces of the housing. In many of these applications the noise performance of the oscillator is a very important consideration. For example, in a doppler radar, noise generated at baseband frequencies that is noise generated at the frequencies of the order of expected doppler frequency shifts, will reduce the subclutter visibility of the radar. In each of the applications mentioned above, the YIG filter or the magneticallly tuned resonant circuit contributes to the noise induced in the circuit. This contribution is particularly important when the other components in the particular circuit are low noise components. Therefore, it is desirable to provide microwave tunable oscillators having very low noise characteristics. One known noise problem is referred to as microphonics and is the noise produced in an output signal in response to an externally applied mechanical force. A YIG filter in a vibrating environment is subject to external forces which cause small dynamic mechanical distortions of the YIG filter housing and, as a result, changes in the magnetic permeability of the magnetically permeable portion of the filter. US-A-4 651 116 describes a magnetically tuned resonant circuit, of the kind defined hereinbefore at the beginning, which includes a housing which provides a magnetic flux return loop. A central post of the circuit includes a pair of pole pieces, upper and lower portions of the housing, and a magnet. Between the pair of pole pieces a radio frequency structure including a pair of coupling loops and a YIG sphere is disposed. A coil is disposed around the pole piece of the upper housing portion and is used to tune the filter to a predetermined resonant frequency. A nonmagnetic, hollow cylindrical member is provided to surround the upper pole piece and protrude beyond the surface of the upper pole piece so that a predetermined gap is provided between the surface of the upper pole piece and the radio frequency structure. The cylindrical member reduces change in resonant frequency caused by externally applied mechanical forces. To substantially eliminate eddy current flow induced in the cylindrical member by the changing radio frequency magnetic field associated with the coupling of resonant frequency energy through the circuit, the material of the cylindrical member is chosen to be nonconductive. Alternatively a cylindrical member having a slit to interrupt the path, or a plurality of spaced members may be disposed between the radio frequency structure and the upper polepiece. In "Advances in YIG-tuned Gunn effect oscillators" at pages 25/4 1-4 of 1972 Wescon Technical Papers, Volume 16, (Los Angeles, 19th-22nd September 1972), B. Oyatuso and Don Zangrando describe a Gunn diode oscillator using a magnetically tuned resonant circuit. The Gunn diode is mounted on a first conductive member, which serves as a cathode connection for the Gunn diode. A second conductive member, which supports a holder for a YIG sphere serving as the gyromagnetic member, acts as part of the anode connection to the Gunn diode, another part of this connection being formed by a diode loop conductor. The diode loop conductor and an output loop conductor are located orthogonally so that coupling between the two loops is null in the absence of the YIG sphere. Nonlinearities in the dynamic tuning are attributed to hysteresis and eddy currents flowing in the polepieces and radio frequency circuit. These effects are said to be minimized by the use of low coercivity and high resistivity materials. Eddy currents may further be reduced by using laminated structures. According to the present invention, a magnetically tuned resonant circuit of the kind defined hereinbefore at the beginning is characterised in that the magnetically inert body member has means for reducing eddy current flow therein. In a preferred embodiment of the present invention, the means for reducing eddy current flow includes means for reducing the electrical conductivity of the magnetically inert member, and that member provides support for the gyromagnetic body. The electrical conductivity of the magnetically inert member is reduced by fabricating the body of the magnetically inert member from a high resistivity material, preferably a dielectric material. Optionally, the body may be provided with a coating of an electrically conductive material. Preferably, the coating has a thickness in the range of about one to ten skin depths, preferably less than four skin depths at the microwave frequency of operation. Preferably still, the electrical conductivity of the magnetically inert member is reduced by breaking the electrical continuity of its structure. With this particular arrangement by substantially reducing the conductivity of the magnetically inert member, induced eddy current flow in the magnetically inert member around the resonant body, and the magnetic field variations concomitant therewith are also reduced. Reduction in magnetic field variations through a YIG sphere which serves as the gyromagnetic member will reduce the variations in resonant frequency of the magnetically tuned resonant circuit. In accordance with a still further aspect of the preferred embodiment the means for providing a magnetic flux path includes a pair of pole caps which provide the pair of opposing spaced surfaces, said caps being comprised of a ferrite material with said caps being disposed adjacent the resonant body. Preferably, the caps are coated with an electrically conductive material having a thickness of about one to ten skin depths preferably less than four skin depths at the microwave frequency of operation. With such an arrangement, by providing a pair of ferrite pole caps to form the pair of opposing, spaced surface portions of a closed flux return path, the ferrite pole caps will provide a high resistance to flow of eddy currents and thus, reduced variations in magnetic flux. Thus, the reduced magnetic flux variations in the region through which the YIG sphere is disposed will provide lower variations in the resonant frequency of the magnetically tuned resonant circuit. In accordance with a still further aspect of the preferred embodiment, the diameter of an aperture provided in the magnetically inert member is at least five times the diameter of a gyromagnetic sphere disposed through the aperture. With this arrangement, by increasing the diameter of the aperture, the sphere will be removed from the proximity of metal sidewalls of the aperture in the magnetically inert member. Hence, currents induced in these conductive sidewalls will provide substantially reduced variations in the magnetic flux directed through the gyromagnetic body. In accordance with an additional aspect of the present invention, an oscillator includes means for providing an electrical signal having a predetermined amplitude and means for feeding a portion of said electrical signal back to the input of said amplitude means. The feedback means includes means including a magnetically tuned resonant circuit, for providing a predetermined phase characteristic to said signal. The magnetically tuned resonant circuit is an embodiment of the invention. With this arrangement, by providing a magnetically tuned resonant circuit having means for reducing variations in resonant frequency, the phase noise imparted to the signal fed therethrough will be reduced, and accordingly the oscillator will have lower frequency modulation noise levels. In accordance with a still further aspect of the present invention, a low noise magnetically tuned oscillator comprises means for providing voltage controlled oscillations and a feedback circuit means, disposed around said voltage controlled oscillation means, including means for detecting frequency noise from the voltage controlled oscillator means and feeding a signal back to said voltage controlled oscillator means in response to said detected noise to cancel the frequency modulation noise in the oscillator. The feedback circuit means further includes a frequency discriminator and a video amplifier. The frequency discriminator includes a magnetically tuned resonant circuit which is used as a dispersive element and a frequency determining element of the oscillator. The magnetically tuned resonant circuit is an embodiment of the invention. With this particular arrangement, since the magnetically tuned resonant circuit is a frequency determining element of the circuit and used to provide a signal which cancels noise in the voltage controlled oscillator, reducing in noise contributed by the magnetically tuned resonant circuit will provide a concomitant reduction in the frequency noise of the microwave oscillator. Brief Description Of The Drawings The foregoing features of this invention, as well as the invention itself may be more fully understood from the following detailed description read together with the accompanying drawings, in which: FIG. 1 is a block diagram of a low noise voltage controlled oscillator employing a magnetically tuned resonant circuit in a frequency modulation noise degeneration loop; FIG. 2 is a cross-sectional view of a YIG tuned band pass filter fabricated in accordance with the present invention, which may be used as the magnetically tuned resonant circuit of FIG. 1; FIG. 3 is an enlarged view of the YIG filter shown in FIG. 2 taken along line 3-3 of FIG. 2; FIG. 4 is a diagrammatical view of a portion of the circuit shown in FIG. 3 taken along line 4-4 of FIG. 3; FIGS. 5A-5E are plots of frequency noise-to-signal ratio vs offset frequency of a conventional YIG filter, and YIG filters fabricated in accordance with the present invention; FIG. 6 is an enlarged view of a portion of a YIG filter similar to that shown in FIG. 2, having conventional pole caps, and an r.f. structure fabricated in accordance with a further respect of the present invention; FIG. 7A is a plan view of the r.f. structure of the YIG filter of FIG. 6; FIG. 7B is a cross-sectional view taken along line 7B-7B of FIG. 7A; FIGS. 8-9 are plan views of alternate arrangements of r.f. structures similar to that of FIG. 6; and FIG. 10 is a block diagram of an oscillator having a magnetically tuned resonant circuit as a frequency determining element disposed in a feedback circuit of the oscillator. Description of the Preferred Embodiments Referring now to FIG. 1, an oscillator 10 circuit is shown to include a magnetically tuned resonant circuit, here a YIG filter 16, used as a dispersive element in an inferometer type of frequency discriminator 28. The discriminator 28 is disposed in the feedback circuit 13 of a voltage controlled oscillator 14. The feedback circuit 13 includes the frequency discriminator 28 and a video amplifier 25. The frequency discriminator 28 includes the YIG filter 16, tuned to the frequency of the oscillator via a control signal fed through the YIG coil driver 26, power divider 18 means 19 for providing a 90° phase shift at the frequency of the oscillator 10 and a phase detector 24 (balanced mixer).The phase detector 24 detects FM noise from the microwave voltage controlled oscillator 14 and converts the detected noise to a baseband voltage. This voltage is amplified by the video amplifier 25, filtered by a shaping filter 17, and sent properly phased to the voltage controlled oscillator to cancel frequency modulation (FM) noise in the oscillator output signal, as is generally known. The lowest noise performance from an oscillator, as shown above, is provided when each of the components are low noise components. However, we have found that one of the most significant contributions to FM noise in such circuits in the magnetically tuned resonant circuit such as the YIG filter 16. Since the frequency of the oscillator signal is directly proportional to the resonant frequency of the YIG filter 16, noise in the YIG filter either from the YIG driver or pass band dither in the resonant frequency of the YIG filter will contribute to FM noise in the oscillator. When there is no danger of onset of spin wave instability, that is, by providing a sphere having a sufficient diameter and by providing sufficient input power to the sphere, the dither in the pass band will then become a significant source of frequency noise. Additive noise is reduced generally by filtering and selection of low noise components. However, noise contributed by dither in the pass band is now reduced as will now be described in conjunction with FIGS. 2-9. Referring now to FIGS. 2-4, a low noise magnetically tuned resonant circuit here a low noise YIG band pass filter 16 is shown to include a composite filter housing 20, having an upper shell portion 20a, an intermediate shell portion 20b, and a lower shell portion 20c. Composite filter housing 20 is comprised of a magnetically permeable material and provides a closed magnetic path or flux return path, to direct magnetic flux through a gyromagnetic member 46 in a manner to be described. Upper shell section 20a includes a first, inner, centrally disposed fixed portion 20a′ having disposed thereon a first pole piece 38, said pole piece 38 having an exposed surface portion 38a. Disposed around portion 20a′ is an electromagnet 40 provided to vary the strength of the D.C. magnetic field H DC , as is known. Lower shell section 120c includes a second, inner, centrally disposed portion 20C′ upon which is disposed a permanent magnet 22 to provide a source of magnetic flux and a second pole piece 24 having an exposed surface portion 24a, as shown. A temperature compensating sleeve 26 is optionally disposed around pole piece 24 and magnet 20, as shown. Intermediate shell portion 20b is shown having disposed over an upper surface portion thereof, a magnetically inert body member which is part of an r.f. structure 30. The r.f. structure 30 is disposed between surface portion 24a of pole piece 24 and surface portion 38a of pole piece 38. The r.f. structure 30 is comprised of a magnetically inert material, as will be described, and includes an aperture portion and a pair of coaxial transmission lines 42, 44. Each one of the coaxial transmission lines 42, 44 include an outer conductor 42a, 44a, dielectrically spaced from a inner conductor 42b, 44b, respectively, as shown. The r.f. structure 30 further includes a body 46 here a sphere comprised of a gyromagnetic material such as yttrium iron garnet (YIG). YIG sphere 46 is disposed on an end portion of a mounting rod (not shown) which is disposed through a passageway (also not shown) provided through the r.f. structure 30. The r.f. structure 30 further includes a pair of coupling loop portions 37a and 37b of central conductors 42b and 44b. The loop portions 37a, 37b are disposed in the aperture 47 and around portions of the YIG sphere 46, with said portions of the YIG sphere 46 being disposed within the coupling loops 37a and 37b. The coupling loops are arranged mutually orthogonal to one another and are spaced from the YIG sphere to provide a requisite amount of coupling to and from the sphere as is generally known in the art. Each one of said coupling loop portions 37a, 37b has end portions coupled to the r.f. structure to provide a short circuit to ground in the region of the YIG sphere 46 to thereby strongly couple to the YIG sphere 46, the r.f. magnetic field component of electromagnetic energy. One of said coupling loops here coupling loop 37a is disposed about the X axis and the second one of said coupling loops 37b is disposed about the Y axis. Therefore, the first coaxial transmission line in the presence of an applied external magnetic field H DC is used to couple a selected portion of said input radio frequency signal to the second one of said coaxial transmission line. The frequency of this coupled radio frequency energy is given in accordance with the equation f₀ =γH DC where f₀ is the resonant frequency of the filter 16, γ is quantity referred to as the gyromagnetic ratio and is approximately equal to 2.8 MHz/Oersted for YIG, and H DC is the magnetic field strength provided through the YIG sphere by the permanent magnet 22. For high performance filters, the pole caps, and r.f. structure are placed under a predetermined compression to reduce vibration induced changes in resonant frequency. Referring now to FIG. 3 and FIG. 4, the pair of pole caps, 24, 38 are shown disposed in the magnetic flux return path. The pole caps 24, 38 comprise a ferrite material 24b, 38b respectively, here having disposed thereover a coating of an electrically conductive material 24a, 38a. The electrically conductive material 24a, 38a preferably comprises a material such as gold or copper, for example and generally has a thickness equal to at least about one skin depth, but generally less than ten skin depths, preferably less than four skin depths at the resonant frequency of the YIG bandpass filter. Accordingly, at the noise frequencies of interest particularly at those of the order of expected doppler frequency shifts, when such a YIG filter is used in a doppler radar receiver, for example, induced magnetic fields resulting from current flow in conductive surfaces of the pole caps will be eliminated because the ferrite is an electrical insulator and, hence, no current will flow. Alternatively, if a conductive coating is provided over the ferrite, such a coating having a thickness of the order of skin depths at the resonant frequency, will provide a high resistivity path to any induced current flow from noise sources at frequencies of the order of 200 KHz or less. Referring to FIGS. 3 and 4, it should also be noted that the r.f. structure 30 is fabricated from a high resistivity material having a resistivity of at least about 100 micro ohm-cm or from a dielectric such as a hard dielectric 30a such as a ceramic. Here the dielectrics portion 30a has disposed thereover a conductive coating 30b of gold and copper, for example, having a thickness of the order of 1-10 skin depths preferably less than four skin depths at the resonant frequency of the YIG filter 16. The high resistivity materials maybe metal alloys, such as cooper, manganese, nickel alloys such as 67Cu-SNi-27Mn, (ρ = 99.75 µohm-cm) nickel base alloys such as 80Ni-20Cr (ρ =112.2 µohm-cm), 75Ni-20Cr-3Au with (Cu or Fe) (ρ = 133 µohm-cm) or iron chromium aluminum alloy such 72Fe-23Cr -5Al-0.5Co (ρ = 135.5 µohm-cm). The hard, refractory dielectrics are ceramics such as alumina (Al₂O) beryllium oxide (BeO) and silica (SiO₂) or other suitable insulating materials. Each of these arrangements reduces the bulk of or the conductivity of the material which provides the r.f. structure 30. Since theoretically derived expressions indicate that H² (magnetic field noise) is inversely proportional to ρ, an increase in ρ will provide a corresponding decrease in the magnetic field noise. That is, the currents induced in the r.f. structure 30 will be weaker due to higher ρ and hence will induce weaker magnetic field fluctuations. Typically, materials chosen for high performance YIG filter r.f. structures are Cu or Cu alloys having resistivities between 1.7 µohm-cm for Cu to 49.88 for 55Cu-45Ni. As also shown in FIGS. 3 and 4, the aperture 47 through which the YIG sphere 46 is disposed has a diameter equal to at least five sphere diameters. With this particular arrangement, since the sphere 46 is relatively isolated from the conductive sidewalls 32 of the aperture 47 in the r.f. structure 30, the sphere 46 will also be isolated from magnetic field variations resulting from currents circulating in these conductive sidewalls. Referring now to FIGS. 5A-5E, system noise as a function of offset frequency for five different pole cap arrangements is shown. Each of these measurements was taken with a test fixture that generally simulated the oscillator described in conjunction with FIG. 1. FIG. 5A shows system FM noise-to-signal ratio versus offset frequency for an oscillator having a YIG filter with conventional pole caps fabricated from a magnetically permeable, electrically conductive material. Here an alloy comprising 80%Ni/20%Fe and generally known as permalloy was used to fabricate the pole caps. FIG. 5B shows FM noise-to-signal ratio vs. offset frequency for the oscillator described above employing a YIG filter as described in conjunction with FIGS. 2 and 3 having pole caps fabricated from a lithium zinc manganese ferrite having an approximate composition in mole ratios of 4/30 Li, 3/30 Zn, 1/30 Mn, with the remainder being Fe. FIG. 5C shows system FM noise-to-signal ratio versus offset frequency for the oscillator arrangement as in FIG. 5B except having a pair of pole caps fabricated from AMPEX (Sunnyvale, CA 94086) part number 3-5000-B which is also a lithium zinc maganese ferrite. FIG. 5D shows system FM noise-to-signal ratio versus offset frequency for the oscillator arrangement as in FIG. 5B, except having pole caps fabricated from Ampex part number RH70-3 which is a zinc maganese ferrite. FIG. 5E shows system FM noise-to-signal versus offset frequency for the oscillator arrangement as in FIG. 5B, except having a pair of pole caps fabricated from alumina. With each of the noise frequency plots shown in FIGS. 5B-5E, the ferrite materials (FIG. 5B-5D) or the magnetically inert, dielectric material (FIG. 5E), is provided with a layer of a conductive material here gold having a thickness of one skin depth at the resonant frequency of the YIG oscillator. A comparison of each of FIGS. 5B-5E with FIG. 5A, therefore, shows that the noise levels are from 2.5 db to 3.0 db lower over the indicated offset frequencies for the YIG filters having pole caps fabricated from electrically insulating, magnetic materials compared to noise level for the conventional permalloy electrically conductive magnetic material arrangement shown in FIG. 5A. Referring now to FIG. 6, a portion of a YIG filter 16′ similar in construction to that of FIG. 2 is shown to include a pair of conventional pole pieces 124, 138 fabricated from an electrically conductive, magnetic material, such as permalloy, having disposed between surfaces 124a, 138a thereof, a modified r.f. structure 130. In particular, r.f. structure 130 may take on any number of configurations, as shown for example in FIGS. 7A through 9. Referring to FIGS. 7A and 7B, modified r.f. structure 130 is shown to include a pair of portions 130a, 130b bonded together, via a nonconductive agent such as epoxy 133 disposed in slots 131a, 131b. The slots 131a, 131b break the electrical continuity around the region through which a YIG sphere 146 is disposed. It is believed that the disruption in electrical continuity prevents eddy current flow around the YIG sphere 146 and eliminates or reduces variations in magnetic fields from this region. Accordingly, there are substantially reduced variations in the magnetic field through the resonant body caused by noise current flow in conductive portions of the r.f. structure 130. Thus, the magnetic field strength through the resonator remains substantially constant as does the frequency and phase characteristics, and the YIG filter 16' with the modified r.f. structure 130 has a substantially lower phase noise and phase variation than conventional YIG filters. When fabricating the YIG filter 16′, care must be taken to prevent the pole caps 124, 138 from contacting the r.f. structure 130 and inadvertently provide an electrical path around the slots 131a′, 131b′. As shown in FIG. 8, a second means for disrupting the electrical continuity or the bulk of conductive material of the r.f. structure is by providing holes 137 here radially through r.f. structure 130. The holes 137 are filled with a dielectric such as air or epoxy or the like; but are provided so that they do not completely sever a portion of the r.f. structure. FIGS. 9A, 9B, show various arrangements of r.f. structure 150, 152 for multi-YIG sphere filters having slots (not numbered) to prevent current flow around the resonators. It is believed that each embodiment of the invention, as described: the ferrite pole caps, 24, 38 having the thin conductive layer; the r.f. structure 130 comprised of a high resistivity material, preferably an electrically insulating material; the r.f. structure having the relatively large aperture within which the YIG sphere is disposed; and the r.f. structure 130 having means provided to interrupt the electrical continuity and prevent current flow around the resonant body; each independently, reduce the phase noise and frequency variations levels of the YIG filter 16, 16′, for example, by reducing the bulk of conductive surfaces proximate to the gyromagnetic member 46. It is believed that induced eddy current flow and in particular thermally induced eddy current flow produces small, random variations in magnetic flux density through the gyromagnetic member 46. Each of the above-mentioned embodiments reduces the magnitude of such eddy current flow in conductive regions adjacent the gyromagnetic member 46 and, hence, reduce the magnitude of the magnetic fields generated by these eddy currents. The ferrite pole caps 24, 28 proximate the resonant body reduce the magnitude of eddy current flow in such pole caps 24, 28, since any eddy current flow is produced only in the thin skin depth conductive coating 24c, 28c. The relatively large aperture isolates the gyromagnetic member 46 from the sidewalls of the cavity 47 provided in the r.f. structure 30 and isolates the gyromagnetic member 46 from magnetic fields which are produced by these currents. The r.f. structure 30 when fabricated from alumina or other high resistivity material, or having a break in the electrical continuity of the r.f. structure, has a reduced magnitude of eddy current flow in the planar conductive surfaces of the r.f. structure. Since this thermally generated eddy current flow induces resonant frequency fluctuation, having rates (within doppler frequency shifts as high as 200 KHz) which lie within the doppler frequency shift of the radar, these embodiments therefore are effective in reducing noise levels of the YIG filter 16 (FIGS. 2-4), 16′ (FIGS. 6-9) at frequencies which correspond to the modulation frequencies of expected doppler frequency shifts in a radar receiver. Hence, use of such a low noise YIG filter in an oscillator application such as shown in FIGS. 1 and 10 in such a doppler radar receiver will increase the subclutter visibility of the radar. Referring now to FIG. 10, an oscillator circuit 160 is shown to include an amplifier 162 disposed in a feedback loop indicated by an arrow 163. Disposed between input and output ports of the amplifier 162 is a feedback circuit including a power divider 164, a low noise magnetically tuned resonant circuit 16 or 16' as described above, and a variable phase shifter 168. The low noise magnetically tuned resonant circuit 16 FIGS. 2-4 (or 16′ FIGS. 6-9), here a YIG tuned bandpass filter, is used to stabilize the phase and frequency characteristics of the oscillator. The output of amplifier 162 is coupled to the input port of the power divider 164. A first output port of power divider 164 is coupled to the resonant circuit 16 and a second output port of the power divider means 164 is coupled to the output terminal 161 of the oscillator 160 and fed to a load (not shown). By using low noise components in the oscillator circuit 160, the output signal fed to terminal 161 will have a frequency spectrum having substantial energy at f c , the center band frequency of the oscillator, with substantially reduced energy at frequencies of at least ± 200 KHz from f c . The frequency of the output signal fed to terminal 161 is provided in accordance with the phase and frequency characteristics of the signal fed back to the input of amplifier 162. The phase and frequency characteristics of the signal are in turn controlled by the phase and frequency characteristics of the YIG tuned filter 16, the phase shifter 168 and the other components in the feedback loop of the oscillator, as is known in the art. Accordingly, by providing the low noise magnetically tuned resonant circuit 16, or 16' in the oscillator, a low noise oscillator 160 is provided.

Claims: A magnetically tuned resonant circuit, comprising: a) means (22, 40) for producing magnetic flux; b) means (20) for providing a magnetic flux path, having a pair of opposing spaced surfaces (24a,38a); c) a magnetically inert member (30) comprising a magnetically inert body member (30a) and disposed between said pair of opposing spaced surfaces (24a, 38a) and having a pair of coaxial conductors (42,44) each having an inner conductor (42b,44b) and an outer conductor (42a,44a) dielectrically spaced therefrom, with the outer conductor (42a,44a) electrically connected to the magnetically inert member (30); and d) a gyromagnetic member (46) disposed in an aperture (47) in said inert body member (30a), with said inert member (30) disposed to have said magnetic flux directed through said gyromagnetic member (46), and the inner conductors (42b,44b) of the said coaxial conductors (42,44) coupled about the gyromagnetic member (46), characterised in that the magnetically inert body member (30a) has means for reducing eddy current flow therein. A circuit according claim 1, characterised in that the means for providing a magnetic flux path includes a pair of members (24,38) disposed adjacent said inert member (30), said pair of members (24,38) providing the pair of opposing spaced surfaces, (24a,38a) and at least one of said pair of members (24,38) being comprised of a magnetically permeable, electrically insulating material (24b,38b). A circuit according to claim 1, characterised in that the means for reducing eddy current flow comprises magnetically inert, electrically insulating material (30a) forming the body of the magnetically inert member (30). A circuit according to claim 3, characterised in that said magnetically inert electrically insulating material (30a) is selected from the group consisting of Al₂O₃, BeO, SiO₂, and in that the magnetically inert body member (30a) has disposed over surfaces thereof, a thin coating (30b) of an electrically conductive material with a thickness in the range of about one to ten skin depths at the resonant frequency of said circuit. A circuit according to claim 1, wherein said means for reducing eddy current flow comprises means (131a,b) interrupting electrical continuity in a region of the inert body member (30a) disposed around the gyromagnetic member (46). A circuit according to claim 5, characterised in that said means for interrupting electrical continuity includes at least one passageway (137) in said magnetically inert structure (130), with said passageway (137) being filled with an electrically insulating material. A circuit according to claim 6, characterised in that said passageway (131a) severs a portion of said member (130). A circuit according to claim 6, characterised in that said passageway (137) is provided through a radial portion of said member (130) and does not sever a portion of said member (130). A circuit according to claim 1, characterised in that the means for reducing eddy current flow comprises a high resistivity material (30a) having a resistivity of greater than about 100 micro ohms-cm forming the body of the magnetically inert member (30). A circuit according to claim 9, characterised in that the high resistivity material is selected from the group consisting of 67 Cu-5Ni-27Mn alloy, 80 Ni-20Cr alloy, 7SNi-20Cr-3Au + remainder Fe or Cu alloy, 75Fe-23Cr-5Al-0.5Co alloy, BeO, Al₂O₃, and S₁O₂. A circuit according to claim 1 or claims 3, characterised in that the means for producing magnetic flux comprises a housing (20) comprised of a magnetically permeable material having the pair of opposing spaced surfaces (24a,38a) provided by a pair of members (24,38) at least one of which is of a magnetically permeable, electrically insulating material. A circuit according to claim 2 or 11, characterised in that said member (24) comprised of the magnetically permeable, electrically insulating material has disposed over surfaces thereof, a coating (24c) of an electrically conductive material. A circuit according to claim 12, characterised in that said magnetically permeable, electrically insulating material (24b) is a ferrite and said coating (24c) has a thickness in the range of about one to ten skin depths at the resonant frequency of said circuit. A circuit according to claim 1 or 11, characterised in that the gyromagnetic member (46) is a sphere having a selected diameter and the said aperture (47) has a diameter equal to at least five times the diameter of said gyromagnetic sphere (46). A low noise oscillator comprising: first means (162), having an input and an output, for providing at the output thereof, an electrical signal having a predetermined amplitude; and second means for feeding a portion of said signal back to said input of the first means (162), further comprising: third means (16,168) for providing a predetermined phase shift characteristic to said signal portion fed back to the input of said amplitude means (162), including a magnetically tuned resonant circuit according to claim 1. An oscillator according to claim 15, characterised in that the magnetically inert member (130) has means (131a,131b) for interrupting electrical continuity in the body of the inert member to prevent eddy current flow around the aperture wherein is disposed the gyromagnetic member (146). An oscillator according to claim 15, characterised in that the means for reducing eddy current flow comprises a high resistivity material having a resistivity of greater than 100 micro - ohms-cm. An oscillator according to claim 17, characterised in that said high resistivity material is selected from the group consisting of Al₂O₃, BeO, SiO₂. A low noise oscillator comprising: means (14) for producing voltage controlled oscillations having a predetermined frequency modulation noise characteristic; and a feedback circuit (13) disposed around said voltage controlled oscillation means (14) including a frequency discriminator (28) incorporating a magnetically tuned resonant circuit according to claim 1.

Inventors: BLIGHT, RONALD E., DIBIASE, ROBERT, GALANI, ZVI, SCHLOEMANN, ERNST F.R.A., WATERMAN, RAYMOND C., JR.
Applicants: RAYTHEON COMPANY
Application year: 1988
Main classification: H01P1
IPC codes: H01P1, H03L7, H01P7