Elastic surface wave device for treating high frequency signals

• US 4,217,564 A
• Filed: 09/15/1978
• Issued: 08/12/1980
• Est. Priority Date: 09/20/1977
• Status: Expired due to Term

• Current Assignee: Thomson-CSF
• Original Assignee: Thomson-CSF
• Inventors: Autran, Jean-Michel
• Primary Examiner(s): Nussbaum, Marvin
• Application Number:
  US05/942,622
• Time in Patent Office: 697 Days
• Field of Search: 333/193-195, 333/196, 333/150-155, 310/313, 331/107 A, 364/821, 330/5.5, 357/25, 357/26
• US Class Current: 333/152
• CPC Class Codes: H03H 9/02779 Continuous surface reflective arrays
• CPC Class Codes: H03H 9/02968 with optical devices mounting in enclosures H03H9/12
• CPC Class Codes: H03H 9/44 Frequency dependent delay lines, e.g. dispersive delay lines

Abstract

The treatment is directly effected on the waves propagated. Zones, for creating interruptions in propagation, are created on the useful surface of the propagation material. Several parallel tracks for propagating the elastic waves are thus delimited by these zones, the length and width of which are selected in dependance upon the required treatment.

Claims

1. An elastic surface wave device for treating high frequency waves forming a filter having a transfer function T(F) of which the inverse Fourier transform I (t), which is the pulse response of the filter, comprises n pulses identical in sign, phase-shifted relative to one another and of various amplitudes which comprises:

A material for propagating said surface waves at a predetermined velocity v, on a useful propagation surface;

input means delivering a front of acoustic waves to be treated to one end, the so-called input end, of the said useful propagation surface of said material;

means, combined with said useful surface, for creating interruptions in propagation in zones where the propagation velocity v'"'"' is different from that v of said material, said zones delimiting n parallel tracks for propagating the elastic waves issuing from said wave front, the width of said zones being proportional to the amplitude of said n pulses and their relative lengths being proportional to the relative phase shifts of said pulses.

2. A device as claimed in claim 1, wherein the said means for creating interruption zones on the surface of said propagation material consist in a treatment of said zones effected on the surface of said material during production of the device.

3. A device as claimed in claim 2, wherein said treatment consists in applying a metallic deposit to said zones, the parameters of this deposit, particularly the type and thickness of metal deposited, determining the relative variations in velocity of the acoustic waves.

4. A device as claimed in claim 2, wherein said treatment consists in implanting ions in said zones, the parameters of this implantation, particularly the type and density of the implanted ions, determining the relative variations in velocity of the acoustic waves.

5. A device as claimed in claim 1, wherein said means for creating interruption zones on the surface of said propagation material comprise a layer of a photoconductive semiconductor material deposited on said surface, the interruption zones appearing through a mask, of which the opening correspond to said zones, when said conductor is illuminated by a light beam.

6. A device as claimed in claim 1, wherein the high frequency waves to be treated consisting of an electrical signal, said input means comprise at least one input transducer.

7. A device as claimed in claim 6, wherein the acoustic waves treated during their propagation along said tracks are collected and converted into an electrical signal by at least one output transducer.

8. A device as claimed in claim 7 forming a filter having a transfer function T (F) of which the inverse Fourier transform I (t), which is the pulse response of the filter, comprises n pulses of given sign and m pulses of opposite sign phase-shifted relative to one another, which comprises:

a first group of n parallel tracks and a second group of m parallel tracks, each of said n+m tracks comprising an interruption zone where the propagation velocity v'"'"' is different from that v of the rest of the useful propagation surface, the width of said zones being proportional to the amplitude of said n+m pulses and their relative lengths being proportional to the relative phase shifts of said pulses;

two wide-band transducers as input and output transducers, the input transducer (or the output transducer) comprising two identical transducers connected in phase opposition.

9. A device as claimed in claim 8, wherein said two groups of n and m parallel tracks are offset perpendicularly to the propagation direction, the two transducers connected in phase opposition being aligned along the direction perpendicular to the propagation direction so that each of them corresponds to one of the two said offset groups.

10. A device as claimed in claim 8, wherein the input transducer emits a front of acoustic waves in the two propagation directions, the two said groups of n and m paralle tracks being situated on either side of this transducer, and the two output transducers being arranged symmetrically in relation to said input transducer so as to receive the waves respectively treated by the two said groups.

11. A device as claimed in claim 7, wherein one and/or the other of the input and output transducers has a predetermined transfer function.

12. A device as claimed in claim 8, wherein material propagating the surface waves being itself dispersive, the interruption zones modify said frequency dispersion of the treated waves.