GB2165411A

GB2165411A - Surface acoustic wave passive transponder having amplitude and phase-modifying surface pads

Info

Publication number: GB2165411A
Application number: GB08425498A
Authority: GB
Inventors: Halvor Skeie
Original assignee: Xcyte Inc
Current assignee: Xcyte Inc
Priority date: 1984-10-09
Filing date: 1984-10-09
Publication date: 1986-04-09
Also published as: DE3438050C2; DE3438050A1; CA1228912A; AU3400284A; GB8425498D0; AU564844B2; JPS61104280A; GB2165411B; ZA847909B; JPH0644039B2

Abstract

A passive transponder for use in an interrogation/transponder system comprises a substrate having a substrate surface 72 defining a path of travel for surface acoustic waves; a launch transducer element 78 arranged on the surface for converting interrogating signals into surface acoustic waves 82 which propagate along the path of travel; a plurality of tap transducer elements 80 arranged on the surface at spaced intervals along the path of travel for converting surface acoustic waves into respective output signals; and a circuit 74,76 connected to the tap transducer elements for combining the output signals therefrom to form reply signals. In order to control the delay time from transducer element to transducer element, one or more "delay pads" 84 are provided on the substrate surface between these transducer elements. <IMAGE>

Description

SPECIFICATION Surface Acoustic Wave Passive Transponder Having Amplitude and Phase-Modifying Surface Pads The present invention relates to a "passive interrogator label system" (PILS); that is a system comprising an interrogator for transmitting an interrogation signal, one or more "labels" or passive transponders which produce a reply signal containing coded information in response to the interrogation signal, and a receiver and decoding system for receiving the reply signal and decoding the information contained therein.

A passive interrogator label system of the type to which the present invention relates is disclosed in the U.S. Patent No.3,273,146 to Horwitz, Jr.; U.S.

Patent No.3,706,094 to Cole and Vaughan; U.S.

Patent No. 3,755,803 to Cole and Vaughan; and U.S.

Patent No.4,058,217 to Vaughan and Cole. In its simplest form, the systems disclosed in these patents include a radio frequency transmitter capable of transmitting RF pulses of electromagnetic energy. These pulses are received at the antenna of a passive transponder and applied to a piezoelectric "launch" transducer adapted to convert the electrical energy received from the antenna into acoustic wave energy in the piezoelectric material. Upon receipt of a pulse, an acoustic wave is generated within the piezoelectric material and transmitted along a defined acoustic path. Further "tap" transducers arranged at prescribed, spaced intervals along this path convert the acoustic wave back into electric energy for reconversion into electrical energy by the launch transducer.The presence or absence of tap transducers at the prescribed locations along the acoustic wave path determines whether a reply pulse will be transmitted with a particular time delay, in response to an interrogation pulse. This determines the information code contained in the transponder reply.

When an acoustic wave pulse is reconverted into an electrical signal it is supplied to an antenna on the transponder and transmitted as RF electromagnetic energy. This energy is received at a receiver and decoder, preferably at the same location as the interrogating transmitter, and the information contained in this response to an interrogation is decoded.

In systems of this general type, the information code associated with and which identifies the passive transponder is built into the transponder at the time that the tap transducers are deposited onto the substrate of piezoelectric material. As mentioned above, the presence or absence of tap transducers at prescribed locations along the acoustic wave paths determines whether a reply pulse will be transmitted with a particular time delay in response to an interrogation pulse. With this type of encoding, the number of possible codes is 2N where N is the number of tap transducers. For a large number of codes, it is necessary to provide a large number of tap transducers; however, increasing the number of tap transducers reduces the efficiency of energy conversion and introduces spurious signals into the reply signal.

It is an object of the present invention to provide a passive transponder adapted for use in an interrogation system for transmitting a reply signal containing encoded information in response to the receipt of an interrogating signal.

It is another object of the present inventionto provide a passive transponder of the above-noted type which comprises a substrate having a substrate surface defining a path of travel for acoustic waves; a launch transducer element arranged on the surface for converting the interrogating signal into an acoustic wave which propagates along the path of travel; a plurality of tap transducer elements arranged on the surface at spaced intervals along the path of travel for converting an acoustic wave into respective output signals; and a circuit, connected to the tap transducer elements, for combining the output signals of these transducer elements to form a reply signal.

It is a further object of the present invention to provide a passive transponder of the above-noted type which permits a large number of codes to be generated with a minimum number of tap tranducers.

These objects, as well as further objects which will become apparent from the discussion that follows, are achieved, according to the present invention, by arranging acoustic wave delay pads on the surface of the substrate along the path of travel of the acoustic wave to control the acoustic wave propagation time from transducer to transducer.

Advantageously, some delay pads are constructed in such a way as to also control the attenuation of the acoustic waves that pass beneath them. To effect this attenuation, at least one edge of such pads is serrated on a side thereof perpendicular to the path of travel of the acoustic wave. The width of the serration in the direction of the path of travel is substantially equal to nA/2 where n is an odd integer and A is the center wavelength of the acoustic waves. Such a serration thus causes portions of the wave which pass beneath the serrated edge to be 1800 out of phase with respect to each other.

The delay pads according to the present invention are utilized in a passive interrogator label system. In this system, the interrogator transmits a first, interrogation signal having a first frequency which successively assumes a plurality of frequency values within a prescribed frequency range. This first frequency may, for example, be in the range of 905--925 MHz, a frequency band which is freely available in many parts of the word for short-range transmission.

The remote, passive transponder associated with this interrogator receives the first signal as an input and produces a second, replay signal as an output.

Signal transforming means within the transponder convert the first signal in such a way as to impart a known informational code in the second signal which is associated with and identifies the particular passive transponder.

Associated with the interrogator of the system is a receiver for receiving the second signal from the passive transponder and a mixer, arranged to receive both the first signal and the second signal, or signals derived therefrom, for mixing together these two signals thereby to produce a further signal. This further signal may, for example, contain the sum and the difference frequencies of the first and second signals, respectively.

Finally, the system includes a signal processor responsive to the signal produced by the mixer for detecting the frequencies contained in this signal thereby to determine the informational code associated with the passive transponder.

For a full understanding of the present invention, reference should now be made to the following detailed description of the preferred embodiments of the invention and to the accompanying drawings.

Fig. is a block diagram of a system for transmitting an interrogation signal, receiving a reply signal and decoding information encoded in the reply signal.

Fig. is a block diagram of a passive transponder adapted for use with the system of Fig. 1.

Fig. 3 is a timing diagram indicating the clock output in the system of Fig. 1.

Fig. 4 is a frequency vs. time diagram illustrating the transmitted signal in the system of Fig. 1.

Fig. 5 is a frequency vs. time diagram illustrating both the transmitted and the received signal in the system of Fig. 1.

Fig. 6 is a plan view, in enlarged scale, of a particular implementation of the transponder of Fig.

2.

Fig. 7 is a plan view, in greatly enlarged scale, of a portion of the implementation shown in Fig. 6.

Fig. 8 is a plan view, in greatiy enlarged scale, of acoustic wave delay pads having serrated edges for controlling the acoustic wave attenuation.

The present invention will now be described with reference to Figs. 1-8 of the drawings. Identical elements in the various figures are designated by the same reference numerals.

Figs. 1-7 illustrate an interrogator-transponder system employing a surface acoustic wave transponder which may form the environment of the present invention. The transmitterlreceiver and decoder system shown in Fig. 1 comprises a ramp generator 20 which supplies a sawtooth waveform to a voltage controlled oscillator (VCO) 22. The VCO produces an output signal offrequencyfwhich repeatedly ramps linearly upward from a frequency of 905 MHz to a frequency of 925 MHz. This signal is amplified by the RF amplifiers 24 and supplied to a transmit'receive switch 26. The switch 26 directs the signal either to a transmitter power amplifier 28 or to a decoding mixer 30.The switch 26 is controlled bya 100 square wave signal produced bya clock 32. The output signal S1 from the amplifier 26 is supplied to an external circulator or transmit" receive (TR) switch 34 and is transmitted as electromagnetic radiation by an antenna 36.

A block diagram of the transponder associated with the system of Fig. 1 is shown in Fig. 2. The transponder receives the signal S1 at an antenna 38 and passes itto a series of delay elements 40 having the indicated delay periods To and AT. After passing each successive delay, a portion of the signal IOI 11, 12 1N is tapped off and supplied to a summing element 111.The resulting signal S2, which is the sum of the intermediate signals IO...IN, is fed back to the antenna 38 for transmission to the antenna 36 in the system of Fig. 1.

The transponder replay signal S2 is received by the antenna 36 and passed through the circulator or TR switch 34to a receiver amplifier 44. The output S4 of this amplifier 44 is heterodyned in the mixer with the signal S3 intermittently presented by the switch 26.

The output S5 of the mixer 30 contains the sum and the difference frequencies of the signals S3 and S4. This output is supplied to a band pass filter 46 with a pass band between 1 and 3 KHz. The output of this filter is passed through an anti-aliasing filter 48 to a sample-and-hold circuit 50.

The sample-and-hold device supplies each ,sample to an analog-to-digital converter 52. The AID converter, in turn, presents the digital value of this sample to a processor 54 that analyzes the frequencies contained in the signal by means of a Fourier transform. The sample-and-hold device 50 and the A/D converter 52 are strobed by a sampling signal which serves to compensate for the non linearity, with respect to time, in the monotonically increasing frequency f of the VCO output signal.

To effect compensation the signal of frequency f produced by the VCO 22 is passed via an isolating amplifier 56 to a delay element 58 with a constant signal delay Ts. Both the delayed and the undelayed signals are supplied to a mixer 60 which produces a signal S7 containing both sum and difference frequencies. The signal S7 is supplied to a low-pass filter 62 which passes only the portion of this signal containing the difference frequencies. The output of the iow-pass filter is supplied to a zero-crossing detector 64 which produces a pulse at each positive (or negative) going zero crossing.These pulses are used to strobe the sample-and-hold device 50 and the A/D converter 52.

Figs. 3--5 illustrate the operation of the circuit of Fig. 1. Fig.3 shows the 100 KHz output of the clock 32; Fig. 4 shows the frequency sweep of the signal produced by the VCO 22. Fig. 5 shows, in solid lines 66, the frequency of the transmitted signal S and, in dashed lines 68, the frequency of the signal S2 as received from the transponder. As may be seen, the signal 68 is received during the interval between transmissions of the signal 66. These intervals are chosen to equal, approximately, the round trip delay time between the transmission of a signal to the transponder and the receipt of the transponder reply. As indicated by the multiple dashed lines, the transponder replay will contain a number of frequencies at any given instant of time as a result of the combined (i.e., summed) intermediate signals having different delay times (To, To+AT, To +2AT,. .To NINT).

Figs. 6 and 7 illustrate an embodiment of a passive transponder which implements the block diagram of Fig. 2. This transponder operates to convert the received signal S, an acoustic wave and then to reconvert the acoustic energy back into an electrical signal S2 for transmission via a dipole antenna 70. More particularly, the signal transforming element of the transponder includes a substrate 72 of piezoelectric material such as a lithium niobate (LiNbQ3) crystal. On the surface of this substrate is deposited a layer of metal, such as aluminum, forming a pattern such as that shown in detail in Fig. 7. For example, this pattern may consist of two bus bars 74 and 76 connected to the dipole antenna 70, a "launch" transducer 78 and a plurality of "tap" transducers 80.The bars 74 and 76 thus define a path of travel 82 for an acoustic wave which is generated by the launch transducer and propagates substantially linearly, reaching the tap transducers each in turn. The tap transducers convert the acoustic wave back into electrical energy which is collected and therefore summed by the bus bars 74 and 76. This electrical energy then activates the dipole antenna 70 and is converted into electromagnetic radiation for transmission as the signal S2.

The tap transducers 80 are provided at equally spaced intervals along the acoustic wave path 82, as shown in Fig. 6, and an informational code associated with the transponder is imparted by providing a selected number of "delay pads" 84 between the tap transducers. These delay pads, which are shown in detail in Fig. 7, are preferably made of the same material as, and deposited with, the bus bars 74,76 and the transducers 78,80. Each delay pad has a width sufficient to delay the propagation of the acoustic wave from one tap transducer 80 to the next by one quarter cycle or 900 with respect to an undelayed wave at the frequency of operation (circa 915 MHz). By providing locations for three delay pads between successive tap transducers, the phase (p of the acoustic wave received by a tap transducer may be controlled to provide four phase possibilities: 1.No pad between successive tap transducers=-90"; 2. One pad between successive tap transducers=0"; 3. Two pads between successive tap transducers=+90"; 4. Three pads between successive tap transducers= + 1800.

Referring to Fig. 2 the phase information o (the phase ofthe signal picked up by the first tap transducer in line), and i, (P2...N N (the phases of the signals picked up by the successive tap transducers) is supplied to the combiner (summer) which in the embodiment of Fig. 6 comprises the bus bars 74 and 76. This phase information, which is transmitted as the signal S2 by the antenna 70, contains the informational code of the transponder.

As shown in Fig. 7, the three delay pads 84 between two tap transducers 80 are each of such a width (L) as to provide a phase delay of 90" in the propagation of an acoustic wave from one tap transducer to the next as compared to the phase in the absence of such a delay pad. This width (L) is dependent upon the material of both the substrate and the delay pad itself as well as upon the thickness of the delay pad and the wavelength of the surface acoustic wave. As noted above, the substrate material is preferably lithium niobate (LiNbO3) and, the delay pad material is preferably aluminum.

In the equations below, V0 equals the propagation velocity of an acoustic wave on a "free surface" without a delay pad (to=3488 meters/second for a lithium niobate substrate); V0=the propagation velocity of an acoustic wave on a surface which is shorted with an infinitely thin delay pad; =the nominal phase delay in the transmission of an acoustic wave from one tap transducer to the following tap transducer when there is no delay pad; and Asp=the additional phase delay imparted by one delay pad. Let us now define:

where K is a "coupling constant" for a metalized (aluminum) piezoelectric (lithium niobate) surface.

Since,

where ktlA is an approximation term due to mass loading by the pad; k is a proportionality constant dependent on the substrate and pad materials; and tis the thickness of the pad, therefore we have,

The preferred thickness of the delay pad film is approximately 0.1 micrometers. The manufacture of the transponder is facilitated if three delay pads are initially deposited between all the tap transducers and, thereafter, delay pads are selectively removed to impart the code to the transponder.

With pads providing a 90" delay, there are four code possibilities for each set of three delay pads.

Consequently, for the transponder illustrated in Fig.

6 having seven sets of delay pads, 47 code possibilities are provided.

Fig. 8 illustrates delay pads 86 which make it possible to control the amplitude as well as the phase of the acoustic wave. Such amplitude modification may be detected by the receiver and decoder system so that additional codes may be imparted in the transponder without requiring additional tap transducers and delay pads.

In this case, the amplitude modification of the surface acoustic wave takes the form of a prescribed attenuation. This attenuation is effected by wave cancellation at the edge of the delay pad.

As is shown in Fig. 8, the serrated edge of the delay pads 86 have a first edge portion 88 and a second edge portion 90 which are perpendicularto the path of travel 92 of the surface acoustic wave but are displaced with respect to each other in the direction of the path of travel by a distance D. The first edge portion 88 has a total length a whereas the second edge portion has a total length b. It will be understood that, whereas the serrated edge is shown to have only two segments in Fig. 8, the edge may be divided into several segments for each edge portion. It is necessary only that the segments of the first edge portion all have a delay pad width L1, whereas the segments of the second edge portion have a delay pad width L2.

Thus, the distance a is the sum of all the first edge portion segments, whereas the distance b is the sum of all the second edge portion segments.

The maximum wave cancellation at the serrated edge is provided when the distance D is selected such thatthe difference in delay provided by the pad at the first and the second edge portion, respectively, is n 180 , where n is an odd integer.

More specifically, D is preferably selected such that -2=nn radians, where (P1, is the additional delay provided by the delay pad over the distance L1, and 2 is the additional delay provided by the delay pad over the distance L2.

From the formula derived above for the width L of a delay pad, we have:

The amount of attenuation provided by the serrated edge may be controlled either by varying the distance D to provide more or less than the optimum delay as defined by the formula above, or by varying the relative total lengths a and 6 of the first and second edge portions. If we let W be the attenuation weighting factor, then W=(a-b)/(a+b) under optimum delay conditions.

As may be seen from this formula, the maximum attenuation occurs when a equals b (W=O). The minimum attenuation occurs when either a orb equals zero (W=1).

It is recommended that the amplitude modifying delay pads 88 be formed in mirror image before and after a tap transducer 94 as illustrated in Fig. 8. This arrangement compensates for irregularities in the acoustic wave front caused by these delay pads.

There has thus been shown and described a novel surface acoustic wave passive transponder, having amplitude and phase-modifying delay pads, which fulfills all the objects and advantages sought therefor. Many changes, modifications, variations and other uses and applications of the subject invention will, however, become apparent to those skilled in the art after considering this specification and the accompanying drawings which disclose preferred embodiments thereof. All such changes, modifications, variations and other uses and applications which do not depart from the spirit and scope of the invention are deemed to be covered by the invention which is limited only by the claims which follow.

Claims

1. In a passive transponder adapted for use in an interrogation system for transmitting a reply signal containing coded information in response to the receipt of an interrogating signal, said transponder comprising: (a) a substrate having a substrate surface defining a path of travel for acoustic waves; (b) a launch transducer arranged on said surface for converting said interrogating signal into an acoustic wave which propagates along said path of travel; (c) a plurality of tap transducers arranged on said surface at spaced intervals along said path of travel for converting said acoustic wave into respective output signals; and (d) circuit means connected to said tap transducers for combining said output signals to form said reply signal; the improvement comprising at least one acoustic wave delay pad disposed on the surface of said substrate along said path of travel to control the acoustic wave propagation time from transducer to transducer.

2. The improvement defined in claim 1, wherein a plurality of said pads are provided, said pads being located between said tap transducers to control the delay time between the respective tap transducers.

3. The improvement defined in claim 2, wherein a plurality of pads are provided between two successive tap transducers.

4. The improvement defined in claim 2, wherein said pads are identical in size.

5. The improvement defined in claim 4, wherein each pad is dimensioned to provide a phase delay of 90" in the acoustic wave.

6. The improvement defined in claim 1, wherein said pad is formed of a metal layer on said surface of said substrate.

7. The improvement defined in claim 6, wherein said metal is aluminum.

8. The improvement defined in claim 1, wherein the width (L) of said pad in the direction of travel of said acoustic wave and the thickness (t) of said pad are selected in accordance with the following formula:

wherein A is the phase delay provided by the pad, A is the center wave length of the acoustic wave, and K0 and k are constants.

9. The improvement defined in claim 8, wherein the phase delay A is 90".

10. The improvement defined in claim 1, wherein at least one edge of said pad is serrated on a side thereof perpendicular to said path of travel, thereby to control attenuation of said acoustic wave.

11. The improvement defined in claim 10, wherein said serrated edge forms first and second edge portions which are perpendicularto said path of travel but displaced with respect to each other in the direction of said path of travel by a distance D such that the difference in delay provided by said pad at said first and second edge portions, respectively, is n 180", where n is an odd integer.

16. Atransponder substantially as hereinbefore described with reference to the drawings.