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Physics of Thermal Wave NDE of Semiconductor Materials and Devices

Published online by Cambridge University Press:  29 November 2013

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Thermal wave physics is playing an ever increasing role in the on-line characterization of semiconductor materials and devices. This is especially true for thermal wave methods that employ laser beams for both the generation and detection of thermal waves. For the modulated reflectance method discussed here, the pump and probe beams are focused on the same spot. They therefore achieve the noncontact advantage of optical methods in addition to the optimum condition for high spatial resolution, a necessary condition for thermal wave measurements on product wafers.

When a material is excited with an intensity-modulated laser beam or pump, a thermal wave is generated in the material and in the air above the sample. The material within this heated region will undergo a thermal expansion which can be detected with a probe beam interferometer or by deflecting the probe beam from the thermoelastic deformation of the surface. Since the complex refractive index of most materials depends on temperature, a modulated temperature will also induce a corresponding modulation in the refractive index and consequently a modulation on a probe beam passing anywhere near the thermal wave. A probe beam directed along the heated surface of the sample, for example, will be deflected as it passes through the heated region above the surface. This mirage effect can also be observed within the sample by directing a transmitting probe through the heated region beneath the surface. Likewise, using a probe beam directed onto the sample surface one can observe a modulation in reflection, transmission, or scattering. A related noncontact method is the photothermal measurement of infrared radiation emitted from the material's heated region. Note that with all these detection methods, thermal wave measurements can be, and most often are, done in air and at room temperature.

Type
On-Line Nondestructive Evaluation
Copyright
Copyright © Materials Research Society 1988

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References

1.Rosencwaig, A., in VLSI Electronics: Microstructure Science 9, edited by Einspruch, N.G. (Academic Press, Orlando, FL, 1985) p. 227.Google Scholar
2.Ameri, S., Ash, E.A., Neuman, V., and Petts, C.R., Electron. Lett. 17 (1981) p. 337.CrossRefGoogle Scholar
3.Olmstead, M.A., Amer, N.M., Kohn, S.E., Fournier, D., and Boccara, A.C., Appl. Phys. A 32 (1983) p. 141.CrossRefGoogle Scholar
4.Olmstead, M.A. and Amer, N.M., J. Vac. Sci. Technol. B 1 (1983) p. 751.CrossRefGoogle Scholar
5.Rosencwaig, A., Opsal, J., and Willenborg, D.L., Appl. Phys. Lett. 43 (1983) p. 166.CrossRefGoogle Scholar
6.Opsal, J., Rosencwaig, A., and Willenborg, D.L., Appl. Opt. 22 (1983) p. 3169.CrossRefGoogle Scholar
7.Fournier, D. and Boccara, A.C., in Scanned Image Microscopy, edited by Ash, E.A. (Academic Press, London, 1980) p. 347.Google Scholar
8.Jackson, W.B., Amer, N.M., Boccara, A.C., and Fournier, D., Appl. Opt. 20 (1981) p. 1333.CrossRefGoogle Scholar
9.Murphy, J.C. and Aamodt, L.C., Appl. Phys. Lett. 38 (1981) p. 196.CrossRefGoogle Scholar
10.Skumanich, A., Fournier, D., Boccara, A.C., and Amer, N.M., Appl. Phys. Lett. 47 (1985) p. 402.CrossRefGoogle Scholar
11.Rosencwaig, A., Opsal, J., Smith, W.L., and Willenborg, D.L., Appl. Phys. Lett. 46 (1985) p. 1013.CrossRefGoogle Scholar
12.Rosencwaig, A., Opsal, J., Smith, W.L., and Willenborg, D.L., J. Appl. Phys. 59 (1986) p. 1392.CrossRefGoogle Scholar
13.Luukkala, M., in Scanned Image Microscopy, edited by Ash, E.A. (Academic Press, London, 1980) p. 273.Google Scholar
14.Busse, G., Scanned Image Microscopy, edited by Ash, E.A. (Academic Press, London, 1980) p. 341.Google Scholar
15.Nordal, P.E. and Kanstad, S.O., in Scanned Image Microscopy, edited by Ash, E.A. (Academic Press, London, 1980) p. 331.Google Scholar
16.Opsal, J. and Rosencwaig, A., Appl. Phys. Lett. 47 (1985) p. 498.CrossRefGoogle Scholar
17.Opsal, J. and Rosencwaig, A., Photoacoustic and Photothertnal Phenomena, Springer Series in Optical Sciences, Vol. 58, edited by Hess, P. and Pelzl, J. (Springer-Verlag, Berlin-Heidelberg, 1988) p. 224.CrossRefGoogle Scholar
18.Smith, W.L., Rosencwaig, A., and Willenborg, D.L., Appl. Phys. Lett. 47 (1985) p. 584.CrossRefGoogle Scholar
19.Smith, W.L., Hahn, S., and Arst, M., in Semiconductor Silicon 1986, edited by Huff, H.R., Abe, T., and Kolbesen, B. (Electrochem. Soc., Pennington, NJ) p. 206.Google Scholar
20.Geraghry, P. and Smith, W.L., in Plasma Processing, edited by Coburn, J., Gottscho, R.A., and Hess, D.W. (Mater. Res. Soc. Symp. Proc. 68, Pittsburgh, PA, 1986) p. 387.Google Scholar
21.Smith, W.L., Rosencwaig, A., Willenborg, D.L., Opsal, J., and Taylor, M.W., Solid State Tech. 29 (1) (1986) p. 85.Google Scholar
22.Weaklim, H.A. and Redfield, D., J. Appl. Phys. 50 (1979) p. 1491.CrossRefGoogle Scholar
23.Opsal, J., Taylor, M.W., Smith, W.L., and Rosencwaig, A., J. Appl. Phys. 61 (1987) p. 240.CrossRefGoogle Scholar