1983
DOI: 10.1063/1.331966
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Fourier transform approach to materials characterization with the acoustic microscope

Abstract: Articles you may be interested inFourier transform approach in modulation technique of experimental measurements Rev. Sci. Instrum. 81, 043110 (2010); 10.1063/1.3327844 Quantum harmonic oscillator revisited: A Fourier transform approach Am. A generalized modal impulse response and Fourier transform approach to investigate acoustic transient Bessel beams and Bessel bullets

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Cited by 31 publications
(10 citation statements)
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“…An inversion algorithm between V(z) and R(B) has been mentioned earlier in optics and is further demonstrated in a work of Hildebrand and Liang [6,7] in acoustics for the reflection coefficient function measurement at liquid-solid interface of substrate materials. We here generalize the method for the layered structure problem where the reflection coefficient function R( BJ) is not only an incident angle dependent function but also a frequency dependent one.…”
Section: Inversion Algorithm To Obtain the Reflection Coefficient R(bmentioning
confidence: 99%
See 1 more Smart Citation
“…An inversion algorithm between V(z) and R(B) has been mentioned earlier in optics and is further demonstrated in a work of Hildebrand and Liang [6,7] in acoustics for the reflection coefficient function measurement at liquid-solid interface of substrate materials. We here generalize the method for the layered structure problem where the reflection coefficient function R( BJ) is not only an incident angle dependent function but also a frequency dependent one.…”
Section: Inversion Algorithm To Obtain the Reflection Coefficient R(bmentioning
confidence: 99%
“…The weighting function can be considered as the multiplication of the direct and inverse pupil function of the acoustic lens and it can be obtained by (5) where F-1 is the inverse Fourier transform operation and Vg(z), called the probe's geometrical response, is a V(z) response corresponding to that obtained from an ideal reflection having R(p) '" 1 for any incident angle and frequency. So we can get the R(P) under normalized form: (6) Knowing that k, = ~ k~ -1[2 p2 and k, = ko sin B, we obtain the reflection coefficient R( B)…”
Section: Inversion Algorithm To Obtain the Reflection Coefficient R(bmentioning
confidence: 99%
“…In acoustic microscopy, the low frequency of the measured signal ensures that the complex amplitude ofthe resulting signal can be measured directly [Hildebrand et al, 1983]. The defocus signal is commonly referred to as V(z), signifying the variation in transducer output-voltage with defocus distance.…”
Section: Aberration Measurement By Confocal Interferometrymentioning
confidence: 99%
“…To realize this powerful technique, it is necessary to measure both amplitude and phase of the V(z) function. Generally, it is not trivial to measure the phase of high-frequency tone burst signals with accuracy, so a special complicated precision phase measurement system was designed [3].…”
Section: Introductonmentioning
confidence: 99%
“…To realize this powerful technique, it is necessary to measure both amplitude and phase of the V(z) function. Generally, it is not trivial to measure the phase of high-frequency tone burst signals with accuracy, so a special complicated precision phase measurement system was designed [3].Another approach to obtain both amplitude and phase information, is based on the use of a Continuous Wave Reflection SCanning Acoustic Microscope [4,5]. In this device, the Continuous Wave V(z) curve is defmed as…”
mentioning
confidence: 99%