Acoustic Transducer for Acoustic Microscopy

The foregoing and other objects will be more clearly understood from the following description taken in conjunction with the following drawing.

FIG. 1 is a schematic diagram of a typical prior art longitudinally polarized transducer-lens system.

FIG. 2 shows the impulse response of the lens system of FIG. 1.

FIG. 3 shows the impulse response of the lens system of FIG. 1 with the acoustic illumination at the center of the lens minimized.

FIG. 4 shows a linearly shear polarized transducer system in accordance with the one embodiment of the present invention.

FIG. 5 is a schematic view showing the shear waves at the lens within the buffer rod.

FIG. 6 is a schematic view showing the coupling at the face of a spherical lens excited by the shear waves of FIG. 5.

FIG. 7 shows a radially shear polarized acoustic transducer in accordance with another embodiment of the invention.

FIG. 8 shows the acoustic field distribution along the direction of polarization in a plane at 0.3 mm defocus, for a linearly-polarized shear transducer lens system.

FIG. 9 shows the impulse response of the radially polarized shear transducer-lens system.

FIG. 4 shows a shear-polarized transducer lens system in accordance with one embodiment of the invention. The system shown includes a buffer rod 11 of quartz, sapphire or silicon, a shear polarized piezoelectric material 12 deposited or suitably attached to one end 13 of the buffer rod. The opposite end 14 of the buffer rod is ground or otherwise formed into a spherical lens 16. Application of voltage across said shear polarized piezoelectric material excites shear polarized waves in the buffer rod as shown by the arrow, which travel downwardly to the lens. The lens is illuminated by the shear polarized acoustic waves 18, FIG. 5. Mode conversion at the buffer rod coupling medium interface excites longitudinal waves in the coupling mediums, usually water, as shown schematically in FIG. 6. Mode conversion will only couple longitudinal waves into the coupling medium at selected locations of the lens. At point "a" no mode conversion takes place because of the normal incidence of the shear wave at the interface. At locations "b" and "c" no longitudinal waves are mode converted because the shear wave is incident on the interface as a shear horizontal polarized wave which couples no energy into longitudinal waves in the coupling medium, and is wholly reflected inside the buffer rod. However, at locations "d" and "e" the shear wave is incident as a shear vertical polarized wave and couples energy into the coupling medium. Thus as shown schematically in FIG. 6, the pattern of excitation of longitudinal waves in the coupling medium is directional in that the energy is excited preferentially along one axis(in the direction of the shear polarization) and is totally absent along the orthogonal axis. With such a transducer-lens combination there is a focal spot with spacial resolution determined by the spherical lens and unidirectionally given by the mode conversion from shear into longitudinal waves at the buffer rod coupling medium interface. With such a lens it is possible to measure anisotropy with a much better spacial resolution than is presently available with a cylindrical lens.

The deposited piezoelectric film may be a film such as zinc oxide with shear polarization and capable of operating at frequencies in the tens of gigahertz range. Thus the method is not restricted to low frequencies but can also be used at any frequency of operation where acoustic microscopes are being made.

Another configuration of a transducer lens system is shown in FIG. 7. The configuration of the piezoelectric material is one which provides radial shear polarized waves shown by the radial arrows in the buffer rod by application of a voltage to the transducer. With such a lens illumination, there are no longitudinal waves converted in the water at the center of the lens. Away from the center of the lens more energy is coupled into the coupling medium by mode conversion. This is because the incidence angle at different locations of the interface vary, with r/F where r is the radial distance from the center of lens and F is the focal length of the lens. If this transducer-lens system is used to measure a sample we find that as the transducer is brought closer to the sample, surface acoustic waves are excited and specular reflections from the sample are very weak and almost nonexistent. With such a transducer acoustic microscopy measurements of surface wave velocity changes with spacial resolution corresponding to a few wavelength of the longitudinal wave in water may be made. In other words, because there are no normal components in the acoustic beam in the coupling medium, a slight defocus (the lens closer to the sample) allows the excitation of surface waves. This excitation is shown in FIG. 8 where amplitude of the acoustic field as a function of distance in terms of x/.lambda. is shown at a focal distance of -0.3 mm at f=50 mHz. It is seen that the distance between peaks is about 8 wavelengths providing a small spot size on the order of a few wavelengths.

The calculations for such a lens is shown in FIG. 9 for a shear transducer-lens system with the frequency equal to 50 MHz defocused 1.8 mm, the diameter being 2 mm and F number 1.65. The sample is hot pressed silicon nitride. FIG. 9 shows clearly that the specularly reflected signal is negligible compared to the surface wave component. This allows one to obtain a clean surface wave with little defocusing, which is very important for material characterization with high spacial resolution.

To take advantage of the "cleaner" surface wave excitation and anisotropic property of the shear transducer-lens system many novel applications can be expected such as measuring the surface wave velocity, residual stress and anisotropy of materials as well as film thickness and subsurface crack depth with good spacial resolution.

The polarized transducer 12 can be made such that both longitudinal and shear waves are excited in the buffer rod. Thus, both types of waves can be used to analyze a specimen and provide different temporal signals.

Thus there has been provided a shear acoustic transducer-lens system for providing high efficiency surface wave excitation. The novel configuration of the shear transducer-lens systems makes it possible to make quantitative measurements of surface wave velocity variations, anisotropy, residual stress, surface defects with a spacial resolution of a few wavelengths of the longitudinal wave in the coupling medium (water).