FREQUENCY-DIVIDING TRANSPONDER AND USE THEREOF IN A PRESENCE DETECTION SYSTEM

Abstract: A batteryless, portable, transponder useful in a tag for a presence detection system. The transponder detects electro­ magnetic radiation at a first predetermined frequency and re­ sponds to said detection by transmitting electromagnetic rad­ iation at a second frequency that is a subharmonic of the first frequency. The transponder includes an amorphous magnetic material component (48) for storing energy from the electro­ magnetic radiation detected at the first frequency for trans­ mission as the electromagnetic radiation transmitted at the second frequency. In one embodiment (Figure 9A), the trans­ ponder includes a thin, flat ribbon (48) of low coercivity mag­ netostrictive amorphous magnetic material having a trans­ verse uniaxial magnetic anisotropy defining a magneto­ mechanical resonant frequency "f" in accordance with the dimensions of the ribbon, when in the presence of a magnetic bias field of a predetermined intensity, wherein the ribbon responds to the detection of electromagnetic radiation having a frequency "2f" by transmitting electromagnetic radiation at a subharmonic of the frequency "2f"; and means for biasing the ribbon with the predetermined magnetic bias field. In an­ other embodiment (Figure 1), the transponder consists of a single resonant circuit including a nonlinear inductor (L1) hav­ ing a core made of amorphous magnetic material; and a cap­ acitance (C1) connected in series with the inductor to define the resonant circuit. The core of the nonlinear inductor inclu­ des an elongated thin, flat ribbon of low coercivity amorphous magnetic material. It has been observed that this resonant circuit exhibits a bifurcated frequency-division characteristic in relation to the amplitude of the detected electromagnetic radiation at the first predetermined frequency, whereby addit­ ional frequency divisions occur as the amplitude is increased. A coded tag (Figure 10) includes two amorphous magnetic material transponders (60, 62) that detect electromagnetic radiation at different frequencies.

Description: The present invention generally pertains to frequency-dividing transponders and is particularly directed to an improved transponder for use in a presence detection system. A presence detection system utilizing a frequency divider as a transponder is described in United Kingdom Patent Application No. 2,017,454. Such system includes a transmitter for transmitting a scanning signal at a first frequency in a surveillance zone; a transponder including an active frequency divider for detecting electromagnetic radiation at the first frequency and for transmitting a presence signal in response thereto at a second frequency to thereby detect the presence of the transponder in the surveillance zone. The electronic tags that the transponders are contained within are attached to articles of which detection is desired for enabling detection of the presence of such articles in the surveillance zone. Such presence detection systems are useful for detecting shoplifting, as well as for other applications. A few examples of such other applications include detecting the presence of a person or vehicle carrying a transponder in a surveillance zone; detecting the presence of articles bearing transponders within a surveillance zone along an assembly line; and detecting the presence of keys attached to transponders in a surveillance zone at the exit of an area from which such keys are not to be removed. The transponder is encased in a small tag that can be attached to an article in such a manner that it cannot be removed from the article without a special tool. When used in a shoplifting detection system, a sales clerk uses a special tool to remove the tag from the merchandise that is paid for; and the surveillance zone is located near the doorway for enabling detection of articles from which the tags have not been removed. The transponder described in the aforementioned patent application includes a complex frequency divider that must be powered by an expensive long-life miniature battery. A frequency divider that may be operated without a battery or any external power supply and is suited for use as a transponder in a presence detection system is described in U.S. Patent No. 4,481,428. Such frequency divider includes a first circuit that is resonant at a first frequency for receiving electromagnetic radiation at the first frequency; a second circuit that is resonant at a second frequency that is a subharmonic of the first frequency for transmitting electromagnetic radiation at the second frequency; and a semiconductor switching device having gain coupling the first and second circuits for causing the second circuit to transmit electromagnetic radiation at the second frequency solely in response to unrectified energy at the first frequency provided in the first circuit upon receipt of electromagnetic radiation at the first frequency. Nonlinearities such as those due to saturation and hysteresis in the magnetization curves of thin magnetic alloy ribbons, including permalloy and untreated Metglas, are well-suited for producing higher-order harmonics, and this effect is described in French Patent No.763,681 to Picard and U.S. Patent No.4,298,862 to Gregor, et. al. In the latter Patent, an amorphous magnetic metal marker in the form of a strip is secured to an article for passage through an incident field in an interrogation zone. However, the marker is capable of producing only magnetic fields which are multiple harmonics of the frequency of the incident field. It is not believed possible to be able to create sub-harmonics and frequency-division behaviour with such ribbons by utilizing only the inherent nonlinearities of their magnetization curves. According to the invention there is provided a batteryless, portable, transponder for detecting electromagnetic radiation at a first predetermined frequency and responding to said detection by transmitting electromagnetic radiation at a different second frequency that has a predetermined relationship to the first frequency, comprising an amorphous magnetic material component for storing energy from the electromagnetic radiation detected at the first frequency for transmission as the electromagnetic radiation transmitted at the second frequency, characterized in that there is provided an elongated, low coercivity magnetostrictive amorphous magnetic material component having a transverse uniaxial magnetic anisotropy defining a magnetomechancial resonant frequency "f" in accordance with the dimensions of the component, when in the presence of a magnetic bias field of a predetermined intensity, wherein the component responds to the detection of electromagnetic radiation having a frequency "2f" by transmitting electromagnetic radiation at a subharmonic of the frequency "2f". The invention provides an improved portable, batteryless transponder that is useful in a presence detection system. The improved frequency divider of the present invention is less complex and less expensive that the frequency divider described in the aforementioned U.S. Patent No.4,481,428, as well as being smaller, lighter and easier to conceal. In one preferred embodiment of the present invention, the amorphous magnetic material component is a thin, flat ribbon; and the transponder includes means for biasing the ribbon with the predetermined magnetic bias field. "Magneto-mechanical" is characteristic of the uniaxial magnetic anisotropy that is necessary for a large interaction between stress and strain and the orientation of the magnetic moment within the ribbon. In another preferred embodiment, the transponder includes a single resonant circuit including a nonlinear inductor having a core made of amorphous magnetic material; and a capacitance connected in series with the inductor to define a resonant circuit that detects electromagnetic radiation at a first predetermined frequency and responds to said detection by transmitting electromagnetic radiation at a second frequency that is a subharmonic of the first frequency. In one preferred embodiment of the single resonant circuit transponder, the resonant circuit further includes a second inductor connected in series with the nonlinear inductor and the capacitance to define the resonant circuit and having a coil that is positioned so that the second inductor is not mutually coupled to the nonlinear inductor. The resonant circuit may consist of either the nonlinear inductor and the capacitance or the nonlinear and second inductors and the capacitance. In a preferred embodiment of the frequency divider, wherein the core of the nonlinear inductor includes an elongated thin flat ribbon of low coercivity amorphous magnetic material, it has been observed that the resonant circuit exhibits a bifurcated frequency-division characteristic in relation to the amplitude of the detected electromagnetic radiation at the first predetermined frequency, whereby additional frequency divisions occur as the amplitude is increased. This bifurcation characteristic is utilized in a preferred embodiment of a presence detection system according to the present invention that uses a tag containing such embodiment of the frequency divider. Additional features of the present invention are described with relation to the description of the preferred embodiments. BRIEF DESCRIPTION OF THE DRAWING Figure 1A illustrates one preferred embodiment of the frequency divider of the present invention. Figure 1B is an equivalent circuit of the frequency divider of Figure 1A. Figure 2A illustrates an alternative preferred embodiment of the frequency divider of the present invention. Figure 2B is an equivalent circuit of the frequency divider of Figure 2A. Figure 3A shows a waveform H of the electromagnetic radiation at the first predetermined freqeuncy detected by the nonlinear inductor at a first amplitude of said detected electromagnetic radiation and a waveform I of the current flowing in the frequency divider of Figure 1A when said first amplitude of eletromagnetic radiation at the first frequency is detected by the nonlinear inductor. Figure 3B shows the frequency spectrum for the electromagnetic radiation transmitted by the frequency divider of Figure 1A in response to detection of electromagnetic radiation of the first amplitude as shown in Figure 3A. Figure 4A shows a waveform H of the electromagnetic radiation at the first predetermined frequency detected by the nonlinear inductor at a second amplitude of said detected electromagnetic radiation greater than that shown in Figure 3A and a waveform I of the current flowing in the frequency divider of Figure 1A when said second amplitude of electromagnetic radiation at the first frequency is detected by the nonlinear inductor. Figure 4B shows the frequency spectrum for the electromagnetic radiation transmitted by the frequency divider of Figure 1A in response to detection of electromagnetic radiation of the second amplitude as shown in Figure 4A. Figure 5A shows a waveform H of the electromagnetic radiation at the first predetermined frequency detected by the nonlinear inductor at a third amplitude of said detected electromagnetic radiation greater than that shown in Figure 4A and a waveform I of the current flowing in the frequency divider of Figure 1A when said third amplitude of electromagnetic radiation at the first frequency is detected by the nonlinear inductor. Figure 5B shows the frequency spectrum for the electromagnetic radiation transmitted by the frequency divider of Figure 1A in response to detection of electromagnetic radiation of the third amplitude as shown in Figure 5A. Figure 6 is a frequency-division bifurcation diagram for the frequency divider of Figure 1A as observed on an oscilloscope. Figure 7 is a computer-generated, frequency-division bifurcation diagram based upon a mathematical model of the frequency divider of Figure 1A. Figure 8 is a block diagram of a presence detection system including a frequency divider according to the present invention. Figure 9 illustrates a preferred embodiment of a presence-detection system tag including a transponder according to the present invention. Figure 9A shows the relative positioning of components in the tag of Figure 9. Figure 10 illustrates another preferred embodiment of a presence-detection system tag including a transponder according to the present invention. Figure 10A shows the relative positioning of components in the tag of Figure 10. Figure 11A and 11B illustrates the effects of magnetic bias fields on the amorphous magnetic material ribbons in the tag of Figure 10. Figures 12A and 12B are performance graphs for the tags of Figures 9 and 10 respectively. DESCRIPTION OF THE PREFERRED EMBODIMENTS Referring to Figures 1A and 1B, one preferred embodiment of the frequency divider of the present invention consists of a nonlinear inductor L1, a second inductor L2 and a capacitance C1, all connected in series with each other to define a series resonant circuit. The values of these components are chosen to define a series resonant circuit that detects electromagnetic radiation at a first predetermined frequency and responds to said detection by transmitting electromagnetic radiation at a second frequency that is a subharmonic of the first frequency. The nonlinear inductor L1 is constructed by closely winding the required number of turns of insulated wire around a core 10 that includes an elongated thin flat ribbon of low-coercivity amorphous magnetic material, such as an alloy sold by Allied-Signal Inc. of Morristown, New Jersey that is identified as "METGLAS 2714A". METGLAS is a trademark of Allied-Signal Inc. In order to achieve the very low demagnetizing factor necessary for operation, the ratio of the overall length of the ribbon 10 to the square root of the cross-sectional area of the ribbon should be at least one-hundred-fifty to one. The coil of the second inductor L2 is wound around the perimeter of the circuit as shown in Figure 1A, and is positioned so as not to mutually couple the second inductor L2 to the nonlinear inductor L1. An alternative preferred embodiment of the frequency divider of the present invention is shown in Figures 2A and 2B. This embodiment consists of a nonlinear inductor L3 and a capacitance C4 connected in series with each other to define a series resonant circuit. The values of these components are chosen to define a series resonant circuit that detects electromagnetic radiation at a first predetermined frequency and responds to said detection by transmitting electromagnetic radiation at a second frequency that is a subharmonic of the first frequency. The nonlinear inductor L3 is constructed in the same manner as the nonlinear inductor L1 in the frequency divider shown in Figures 1A and 1B. The frequency divider of Figure 2A is not as efficient as the frequency divider of Figure 1A because of a smaller capture area; but it is simpler and less costly to manufacture. The following discussion pertains to a possible theory of operation of the frequency divider of the present invention. Figure 3A shows the relative amplitude of a waveform H of the electromagnetic radiation at the first predetermined frequency detected by the nonlinear inductor and a waveform I of the current flowing in the resonant circuit of Figure 1A. Figure 3B is the corresponding frequency spectrum of the current in the resonant circuit of Figure 1A. In a similar manner, Figures 4A and 4B and 5A and 5B show the result of increasing the amplitude of the interrogating electromagnetic field. The circuit of Figure 1A undergoes progressive stages of frequency division as a function of the amplitude of the detected electromagnetic radiation at the first predetermined frequency and eventually reaches the chaotic state shown in Figures 5A and 5B. A recent theory by M. J. Feigenbaum (J. Stat, Phys. 19, page 25, 1978 and Feigenbaum, J. Stat, Phys. 21, page 665, 1979), regarding nonlinear systems which exhibit period-doubling, predicts that these systems should behave in a universal manner independent of the precise equations which govern their dynamics. In Physical Review Letters, Vol.47, No.19 pp.1349-52, Nov.1981 P.S. Lindsay summarizes Feigenbaum's theory as follows: Consider a system described by the coupled differential equations. dx;/dt + F i (X₁, X₂,..., X n , λ), i=1,2...,n (Eq.1) The X i (t) are periodic with period T n =2 n T₀ at λ =λ n . For example in the circuit of Figure 1A, the X i correspond to charge and current flowing in the circuit and λ is the amplitude of the driving voltage. The theory predicts that the modulation parameter, λ , should asypmtotically satisfy the recurrence relation (λ n+1 -λ n )/(λ n+2 -λ n+1 ) = δ (Eq. 2) δ is a universal convergence rate that depends only on the nature of F i near an extremum. For a quadratic extremum δ = 4.669....when n is large, the odd components of the Fourier spectrum are related by The quantity X (2k+1) (n) is the complex Fourier amplitude for the frequency (2k+1)/2 n T o and α = 2.5029... is the universal rescaling factor. Once a Fourier component appears at a particular frequency it is predicted that it will remain essentially constant through any succeeding frequency divisions. Figure 6 is a typical real-time bifurcation diagram of the resonant circuit of Figure 1A. This diagram is the result of sampling and displaying the instantaneous current, i(n*T), flowing in the series resonant circuit of Figure 1A at the beginning of each cycle of the detected electromagnetic radiation at the first predetermined frequency on the Y-axis of an oscilloscope. At the same time, the amplitude of the detected electromagnetic radiation at the first predetermined frequency is slowly varied and displayed along the X-axis. The diagram is useful because it clearly reveals threshold values of amplitude for progressive frequency-division bifurcations, convergence rate, rescaling factor, and the onset of chaotic behavior. Bifurcations at f/2, f/4, and f/8 are visible, as well as a window at f/5 in the chaotic region. This behavior may be exploited as a characteristic signature of the invention. A numerical model has been developed to further analyze the circuit of Figure 1A. The flux  B , through the nonlinear inductor L1 is derived from the field generated by the current i(t), flowing through the coil surrounding it and external magnetic field, such as the earth's magnetic field. The external steady magnetic field is equivalent to adding a D.C. component to the current saturating the nonlinear inductor L1. i eq (t) = i(t) + i dc (Eq. 4) This biasing effect adds an asymmetry to the saturation curve of the inductor required for subharmonic generation. In the nonlinear inductor L1 of Figure 1A, the hysterisis effects are small and can be neglected whereby the relationship between  B and i eq is a single-valued function, to wit: if -i c <i eq <i c then  B = M₁ i eq (Eq. 5) if i eq >i c then  B = M₀i eq + (I Bs -M₀i c ) (Eq. 6) if i eq <-i c then  B = M₀i eq - (I Bs -M₀i c ) (Eq. 7)  B is the saturation flux; and i c is the saturation current. In order to solve the circuit equations we must know d B /dt as a function of the current i eq . This is accomplished by differentiating the previous equations and substituting i + i dc for i eq . if -i c <(i+i dc )<i c then d B /dt = M₁di/dt (Eq. 8) if (i+i dc )>i c then d B /dt = M₀di/dt (Eq. 9) if (i+i dc )<-i c then d B /dt = M₀di/dt (Eq. 10) It is now possible to write the differential equations describing the conditions in the resonant circuit of Figure 1A as follows: EsinWt = L₂di/dt + Ri + M(i)di/dt + V c (Eq. 11) i = CdV c /dt (Eq. 12) W is 2π times the frequency of the detected electromagnetic radiation at the first predetermined frequency; E is the amplitude of said detected electromagnetic radiation; R is the wire resistance, and V c is the voltage across the capacitor C1. These are coupled, nonlinear differential equations which may be solved using a numerical technique such as the Runge-Kutta technique to obtain current and voltage as a function of time. Figure 7 is a computer-generated bifurcation diagram using this numerical model, wherein R = 24.4Ω, L2 = 1.28mh, C1 = 2.0mmf, W = 8.0kHz, i dc = 1.1ma and E varies from 0 to 0.45 volts. Above each value E on the horizontal axis, the 16 values i(n*T), for n = 25,26,...,40 are reported. We start with n = 25 to leave time for the solution to reach a steady state, if there is any. If the steady state is periodic with period 2*T then 2 sets of 8 identical points are obtained. This is the first bifurcation. The bias level, i dc , was set equal to i c for this diagram and the result is a very low threshold, with E being approximately equal to 0, for the first bifurcation. This condition is desirable when using the frequency divider of Figure 1A as a transponder contained within an electronic tag in a presence detection system. In practice, the circuit of Figure 1A shows the lowest threshold for bifurcation when the external magnetic bias field is equivalent to the field generated by the saturation current, i c , in the coil wrapped around the amorphous magnetic strip 10 of the nonlinear inductor L1; and the circuit is series resonant at one-half the frequency of the detected electromagnetic radiation at the first predetermined frequency. The biasing magnetic field may simply be the Earth's magnetic field, or a small permanent magnet placed near the nonlinear inductor. This feature is utilized in a preferred embodiment of a presence detection system according to the present invention, as shown in Figure 8. Such system includes a transmitter 20, an electronic tag 22, a detection system 24 and a permanent magnet 26. The transmitter 20 transmits an electromagnetic radiation signal 28 of a first predetermined frequency into a surveillance zone 30. The tag 22 is attached to an article (not shown) to be detected within the surveillance zone 30. The tag 22 includes a batteryless, portable, frequency divider constructed as described above with reference to either Figure 1A or Figure 2A. The permanent magnet 26 provides an external magnetic bias field within the surveillance zone 30 that is equivalent in strength to the magnetic field generated by the saturation current in the coil would around the core of the nonlinear inductor L1 in the frequency divider in response to the detected electromagnetic radiation at the first predetermined frequency. The detection system 24 detects electromagnetic radiation at the second frequency in the surveillance zone 30, and thereby detects the presence of the tag 22 in the surveillance zone 30. The frequency-division bifurcation characteristic of the resonant circuit of Figure 1A is utilized by causing the transmitter 20 to transmit electromagnetic radiation at the first frequency having an amplitude that causes the resonant circuit to transmit electromagnetic radiation at multiple subharmonics of the first frequency. The detection system 24 then must detect electromagnetic radiation 32 in the surveillance zone 30 at one or more of the multiple subharmonics in order to detect the presence of a tag 22 in the surveillance zone 30. The present invention further provides a batteryless, portable, frequency-dividing transponder that includes an elongated thin flat ribbon of low coercivity magnetostrictive amorphous magnetic material that has a traverse uniaxial magnetic anisotropy as a result of having been annealed in a magnetic field that is transverse to the length of the ribbon and in the plane of the ribbon, and which detects electromagnetic radiation having a given frequency and responds to the detection of said radiation by transmitting electromagnetic radiation at a subharmonic of the given frequency of the detected radiation. Such transponder is included in a tag for use in a presence detection system according to the present invention. The uniaxial magnetic anisotropy of the ribbon defines the magnetomechanical resonant frequency characteristic of the ribbon. The ribbon has a characteristic magnetomechanical resonant frequency "f", and responds to detection of electromagnetic radiation having a frequency 2f, by transmitting electromagnetic radiation at a subharmonic of the frequency of the detected radiation. The characteristic magnetomechanical resonant frequency of the frequency-divider ribbon is dependent upon the length of the ribbon, and does not resonate unless in the presence of a magnetic bias field of a predetermined intensity. Two examples of amorphous magnetic materials that can be processed to provide an amorphous magnetic material ribbon that exhibits frequency-division characteristics are Fe₆₇Co₁₈B₁₄Si₁, Fe₈₁B 13.5 Si 3.5 C₂, and Fe₄₀Ni₃₈Mo₄B₁₈ which are sold by Allied-Signal Inc. Corporation of Morristown, New Jersey as METGLAS 2605CO, METGLAS 2605SC and METGLAS 2826MB. It is believed that Fe₈₂B₁₂Si₆ and Fe₇₈B₁₉Si₁₉, which are described Table IV in U.S. Patent No. 4,553,136 to Anderson, III et al., also may be processed as described herein to provide a ribbon that exhibits frequency-division characteristics. The amorphous magnetic material is processed to provide the frequency-dividing transponder ribbon by the following process. First, the material is cut into a long narrow strip so that demagnetizing effects are very small. The cut ribbon is then annealed in the presence of a magnetic field that is transverse to the length of the ribbon and in the plane of the ribbon. A ribbon that has been so processed is referred to herein as a "frequency-divider ribbon". This process creates a transverse uniaxial magnetic anisotropy that is necessary for a large interaction between stress and strain and the orientation of the magnetic moment. It is believed that energy is stored mechanically in the vibrations of the frequency-divider ribbon; whereas in the embodiments of Figures 1A and 2A, energy is stored in a capacitor. Consequently, frequency division can be achieved by the frequency-divider ribbon alone and apart from any other resonant-circuit components. The frequency-divider ribbon has a characteristic mechanical resonant frequency that is expressed by the equation: f r = c H /2L (Eq. 13) wherein "L" is the length of the ribbon and C is the speed of sound in the ribbon. wherein p is the density of the material and S H / 33 is the elastic constant of the ribbon material and is dependent upon the strength of any external magnetic bias field applied to the ribbon. Frequency division does not occur unless an external magnetic bias field within a predetermined field intensity range is applied to the frequency divider ribbon. In one example, METGLAS 2605SC material was cut into ribbons that were approximately 10 cm by 0.2 cm. The material had a thickness, as cast, in a range of about 25 to 38 microns. These ribbons then were annealed in a transverse magnetic field of approximately 5000 Oersteds for ten minutes at approximately 394 degrees Centigrade. The ribbons then were allowed to cool to the ambient temperature with the 5000 Oersted magnetic field still applied. The resultant frequency-divider ribbon was observed to have a characteristic magnetomechanical resonant frequency of approximately 10 kHz when an external magnetic bias field of 0.55 Oersteds was applied thereto. For an external magnetic bias field strength of 0.6 Oersteds, the characteristic magnetomechanical resonant frequency of the ribbon was approximately 9.4 kHz. As the strength of the applied field was increased above 0.6 Oersteds, the amplitude of a voltage signal induced in a coil wrapped around the ribbon of the characteristic magnetomechanical resonant frequency of the ribbon also increased to a peak and then declined to zero. The highest amplitude of the resonant signal was observed when the strength of the applied external magnetic bias field was at the peak of the elastic curve (S H / 33 vs. H), and the frequency of the detected transmitted signal was approximately twice the characteristic magnetomechanical resonant frequency of the frequency-divider ribbon. With a 0.55 Oersted external magnetic bias field applied to the frequency-divider ribbon to produce a 10 kHz characteristic magnetomechanical resonant frequency therein, the highest amplitude subharmonic signal observed was the 10 kHz signal transmitted by the frequency-divider ribbon in response to detection of a 20 kHz transmitted signal. The frequency-divider ribbon is included in the tag 22 in the presence detection system of Figure 8, described above, in place of the frequency divider of Figure 1A or Figure 2A. The frequency of the electromagnetic radiation signal 28 transmitted by the transmitter 20 is approximately twice the characteristic magnetomechanical resonant frequency of the frequency-divider ribbon. The frequency-divider ribbon in the tag 22 detects the transmitted electromagnetic signal 28 and responds thereto by transmitting a signal 32 at a subharmonic of the frequency of the transmitted signal 28. The detection system 24 is tuned to detect a subharmonic, preferably one-half, of the frequency of the transmitted signal 28 to thereby detect the presence of the tag 22 in the surveillance zone 30. In some locations and with some frequency-divider ribbons, the strength of the Earth's magnetic field may be adequate to provide the external magnetic bias field in the surveillance zone 30, whereby the permanent magnet 26 may be omitted. In an alternative embodiment, the tag includes a plurality of frequency-divider ribbons of different lengths, which thereby have different characteristic magnetomechanical resonant frequencies. Different combinations of frequency-divider ribbons are included in different tags to thereby provide uniquely-coded tags. To detect the presence of a coded tag 22 in the surveillance zone 30, the transmitter 20 provides a transmitted signal 28 that is swept over a predetermined range of frequencies that includes each of the frequencies that are twice the characteristic magnetomechanical resonant frequency of each of the frequency-divider ribbons; and the detection system 24 detects signals at each of the characteristic resonant frequencies to detect the presence of the tag 22 in the surveillance zone 30. In another alternative embodiment, the detection system 24 detects an acoustic wave at the characteristic magnetomechanical resonant frequency of the frequency-divider ribbon to detect the presence of the tag 22 in the surveillance zone 30. Figures 9 and 9A show a low-cost version of a frequency-dividing transponder that is useful as an antipilferage tag 40 in a presence detection system. The tag 40 includes a housing 42 defining cavities 44 and 46 for containing an amorphous magnetic material ribbon 48 and a high remenance magnetic alloy ribbon 50, which has a relatively high coercivity compared to the amorphous ribbon 48. The housing 42 includes a paper cover 52, a paper base 54, and paper spacers 56. The amorphous ribbon 48 must be able to vibrate freely inside the housing cavity 44 without interference or restriction, and must have no mechanical stresses impressed on it from the walls of the cavity 44. One exception to this might be to fix the amorphous ribbon 48 with a small bead of silicone adhesive at its center nodal point. The dimensions of a typical amorphous ribbon 48 are 7cm long by 0.25 cm wide by 30µm thick. The dimensions of the cavity 44 need only be slightly larer than the dimensions of the ribbon 48. A suitable bias ribbon material is 0.65 to 1.0 percent carbon steel ribbon with B r =9000 gauss and 2 to 5 mils thick. The amorphous ribbon 48 is biased by a magnetic field provided by the high remenance magnetic alloy ribbon 50. The relative positioning of the two ribbons 48 and 50 is shown in Figure 9A. The distance, d, between the amorphous ribbon 48 and the bias ribbon 50 is adjusted so that the amorphous ribbon is at its optimum threshold for subdivision. The bias ribbon 50 does not need to move freely and can be attached directly to the housing 42 with adhesives or sandwiched between the layers 52 and 54 of the housing 42. The transponder is enabled by permanently magnetizing the bias ribbon 50. The transponder may be disabled by authorized personnel by degaussing the bias ribbon 50 in a high A.C. magnetic field. An important advantage provided by this transponder is that it is not necessary to actually make physical contact with the transponder to deactivate it, so its location is not easily discovered. Figures 10 and 10A show a high performance version of a frequency-dividing transponder that is useful as an antipilferage tag 58 in a presence detection system. This transponder is preferred because its performance is not affected by the interference caused by the Earth's magnetic field. The Earth's magnetic field may be strong enough to significantly degrade the performance of the transponder of Figure 9 if it happens to align with the magnetic field generated by the bias ribbon 50. The amorphous ribbon 48 responds to the sum of the component of the Earth's magnetic field along its length and the magnetic field from the bias ribbon 64. The tag 58 includes a housing 66 defining cavities 68, 70 and 72 for containing the amorphous ribbons 60 and 62 and th bias ribbon 64 respectively. The housing 66 includes a paper cover 74, a paper base 76 and paper spacers 78. The ribbons 60, 62 and 64 are of the same materials and dimensions as used in the transponder of Figure 9. The relative positioning of the ribbons of the transponder of Figure 10 is shown in Figure 10A. One amorphous ribbon 60 is at a distance d₁ from the bias ribbon 64. This amorphous ribbon 60 has an optimum magnetic bias field B₁+B E resulting when the Earth's magnetic field B E is parallel with the length of the ribbon 60 and aiding the field B₁ from the bias ribbon 64. This situation is illustrated in Figure 11A. The other amorphous ribbon 62 is at a distance d₂, which is less than d₁, from the bias ribbon 64. This second amorphous ribbon 62 has an optimum magnetic bias field B₂-B E resulting when the Earth's magnetic field B E is parallel with the length of the ribbon and opposing the field B₂ from the bias ribbon. This situation is illustrated in Figure 11B. The advantage is that either the first amorphous ribbon 60 or the second amorphous ribbon 62 will be biased near its optimum level for frequency division, depending on how the tag 58 is oriented in the Earth's field. Figures 12A and 12B provide a graphical representation of the performance curves of the transponders of Figure 9 and 10 respectively as a function of magnetic field strength H. Performance is measured by the amplitude of the signal at the subharmonic frequency that is transmitted by the transponder. The high performance transponder of Figure 10 may be enabled and disabled in a manner similar to that of the low cost transponder of Figure 9.

Claims: A batteryless, portable, transponder for detecting electromagnetic radiation at a first predetermined frequency and responding to said detection by transmitting electromagnetic radiation at a different second frequency that has a predetermined relationship to the first frequency, comprising an amorphous magnetic material component (48) for storing energy from the electromagnetic radiation detected at the first frequency for transmission as the electromagnetic radiation transmitted at the second frequency, characterized by an elongated, low coercivity magnetostrictive amorphous magnetic material component (48) having a transverse uniaxial magnetic anisotropy defining a magnetomechancial resonant frequency "f" in accordance with the dimensions of the component, when in the presence of a magnetic bias field of a predetermined intensity, wherein the component responds to the detection of electromagnetic radiation having a frequency "2f" by transmitting electromagnetic radiation at a subharmonic of the frequency "2f". A transponder according to Claim 1, wherein the component (48) is a thin, flat ribbon. A transponder according to Claim 2, characterised in that further means (50) is provided for biasing the ribbon (48) with said predetermined magnetic bias field. A transponder according to Claim 2, characterised in that the amorphous magnetic material of the ribbon (48) is selected from a group consisting of Fe₆₇Co₁₈B₁₄Si₁, Fe₈₁B 13.5 Si 3.5 C₂, Fe₄₀Ni₃₈Mo₄B₁₈, Fe₈₂B₁₂Si₆ and Fe₇₈B₁₃Si₁₉. A transponder according to Claim 2, characterised in that a housing (42) is provided defining a cavity (44) that contains the ribbon (48) and enables the ribbon to vibrate freely within the cavity without any restriction being impressed on the ribbon by the housing. A transponder according to Claim 5, characterised in that the housing (42) further contains biasing means (50) for biasing the ribbon with said predetermined magnetic bias field and disposes the biasing means in a predetermined relationship to the ribbon (48) to bias the ribbon with said predetermined magnetic bias field. A transponder according to Claim 1, characterised in that a single resonant circuit is provided comprising a nonlinear inductor (L1, L3) having a core made of amorphous magnetic material; and a capacitance (C1, C4) connected in series with the inductor to define a resonant circuit that detects electromagnetic radiation at a first predetermined frequency and responds to said detection by transmitting electromagnetic radiation at a second frequency that is sub-harmonic of the first frequency. A coded tag (58) for attachment to an article to be detected within a surveillance zone, comprising a first batteryless, portable, transponder (60) for detecting electromagnetic radiation at a first predetermined frequency and responding to said detection by transmitting electromagnetic radiation at a second frequency that is a sub-harmonic of the first frequency, characterised in that there is provided an amorphous magnetic material component for storing energy from the electromagnetic radiation detected at the first frequency for transmission as the electromagnetic radiation transmitted at the second frequency; and in that a second batteryless, portable, transponder (62) is provided for detecting electromagnetic radiation at a third predetermined frequency and responding to said detection by transmitting electromagnetic radiation at a fourth frequency that is a sub-harmonic of the third frequency, the second transporter (62) including an amorphous magnetic material component for storing energy from the electromagnetic radiation detected at the third frequency for transmission as the electromagnetic radiation transmitted at the fourth frequency. A presence detection system, comprising means (20) for transmitting an electromagnetic radiation signal of a first predetermined frequency into a surveillance zone; a tag (22) for attachment to an article to be detected within the surveillance zone, including a batteryless, portable, transponder for detecting electromagnetic radiation at the first predetermined frequency and responding to said detection by transmitting electromagnetic radiation at a second frequency that is a sub-harmonic of the first frequency, and means (24) for detecting electromagnetic radiation at the second frequency within the surveillance zone, characterised in that the transponder comprises an elongated low coercivity magnetostrictive amorphous magnetic material component (48) having a transverse uniaxial magnetic anisotropy defining a magnetomechanical resonant frequency "f" in accordance with the dimensions of the component, when in the presence of a magnetic bias field of a predetermined intensity, wherein the component responds to the detection of electromagnetic radiation having a frequency "2f" by transmitting electromagnetic radiation at a subharmonic of the frequency "2f"; and in that the system includes means (50) for biasing the component with said predetermined magnetic bias field. A system according to Claim 9, wherein the component (48) is a thin, flat ribbon.

Inventors: CHARLOT, LINCOLN H., JR., FERGUSON, LUCIAN G.
Applicants: SECURITY TAG SYSTEMS, INC.
Application year: 1986
Main classification: G08B13
IPC codes: G01S13, G06K7, G08B13