Second-and third-harmonic generation in silicon carbide (SiC) nanopowders embedded in a polymethyl methacrylate (P MMA) film are studied using nano-, pico-, and femtosecond laser pulses. Second-and third-harmonic generation processes are shown to allow the detection of absorptive agglomerates of nanocrystals in transparent materials and the visualization of optical breakdown in nanocomposite materials. Polarization of the third-harmonic signal is shown to be highly sensitive to the polarization of the pump field, permitting third-harmonic generation to be used as a probe for the anisotropy of nanocomposite materials. The second-harmonic signal, on the contrary, has no memory of the initial polarization state of the pump field and is, consequently, ideally suited as a measure of orientation-averaged nonlinearities of nanopowder materials. Second-harmonic yield, arb. un. Nanoscale nonlinear optics [1] unveils the fundamental aspects of light-nanostructured matter interactions and gives recipes for designing new materials and creating novel devices for laser physics, nonlinear optics, and ultrafast photonics. Nonlinear optics also offers equally elegant and convenient methods to understand many of fundamental properties of micro-and nanostructured matter [2,3]. Harmonic-generation and wave-mixing processes have been shown to offer new solutions in nonlinear microscopy. In particular, third-harmonic generation (THG) proved to be a very useful tool for a microscopy of biological objects [4,5] and plasmas [6]. It would be a challenging task to extend the ideas of nonlinear-optical imaging to nanoscale systems by applying harmonic-generation and wave-mixing techniques to the visualization of assemblies of nanocrystals and nanoparticles and analysis of nanocomposite materials.