The noncontact imaging of the buried structures is carried out in the open-air atmosphere by using the photothermal deflection (PTD) method. We applied these techniques to the layered samples. Besides the PTD images for the optically opaque buried structures, the parameters of the materials such as thermal diffusivity can also be calculated from the PTD amplitude and phase signal in the PTD scanning images. When the PTD signals at two different modulation frequencies are used, the thermal diffusivity of the buried structure can be obtained from the PTD signal outside of the sample nondestructively. 78.20.Hp; 42.30.Va; 65.90.+i Recently, the demand for the nondestructive detection method on the optically opaque buried structures has been increasing by the development of complex functional materials. Since the photoacoustic and photothermal phenomena (PPP) were applied to the nondestructive imaging in the early 1980's [1-4], the photoacoustic microscope (PAM) techniques have been used for the observation and the evaluation of both the surface and inner defects [5,6]. The nondestructive evaluations of the grooved metal planes [7] and the simulated pitting corrosions [8] were reported. The thermal parameters can be obtained in the photoacoustic techniques [9]. Thermal diffusivity is obtained from the modulation frequency dependence of photoacoustic signals [10,11]. The thermal properties are analyzed at the plasma-sprayed zirconia coating [12].
PACS:The PPP is used to detect the nonradiative process in the materials. The photothermal deflection (PTD) method is a kind of PPP [13] and it enables us to measure the absorption spectra and thermal properties of the specimen without contact. In the PTD method, chopped monochromatic excitation light is irradiated onto the sample. The change in the refractive index of the atmosphere just above the sample surface is detected by the crossing probe light which is incident on the sample surface at low angle [14]. The excitation beam is scanned through the sample surface by the mechanical stage with a micropositioner, and the photothermal deflection image can be obtained. This method is superior to the other PAM techniques because it does not require samples to be confined in a photoacoustic (PA) cell like the gas-microphone PA spectroscopy, or the sensors to be directly attached to the sample as in the piezoelectrictransducer method. Therefore, the PTD method allows us to study the temperature-dependent photothermal characteristics of the samples directly.In the PTD methods, both amplitude and the phase signals are obtained simultaneously [15], and one can obtain several parameters of the material such as the optical absorption coefficient and the thermal diffusivity. Furthermore, one can get the depth profile of signals by changing the modulation frequency. Although the thermal properties were obtained from the modulation frequency dependence of the PTD signals in the scanned images until now [10,11], we apply the vector model [15] to the scanning imaging methods and calculat...