Third harmonic microscopy of intrinsic and induced material anisotropy in dielectric thin films

Abstract. Third harmonic (TH) microscopy with circularly polarized illumination directly reveals material anisotropy owing to suppression of background optical signals from isotropic media. Because optical thin films and their substrates are expected to be highly isotropic, TH microscopy presents a path to study induced and intrinsic anisotropy in films, providing both insight into laser-induced material modification that precedes damage and feedback about the deposition process. Because nanoscale defects and material strain influence the damage behavior of films, we examined TH sensitivity to similar sources of contrast. We demonstrate imaging of individual 10 nm colloidal gold nanoparticles and 100 mN nanoindentations in fused silica both with signal-to-noise ratio (SNR)≥100∶1. We present TH images (SNR≥210∶1) of sites exposed to femtosecond laser pulses below damage in 100 nm HfO2 films that are barely visible (SNR≤2.3∶1) with Nomarski and polarization imaging, traditional microscopic techniques known to display contrast for material anisotropy. At our detection limit (320 mW, 50 fs, 790 nm, ≈106 photomultiplier tube gain), we examined root mean square in the TH image of nascent films that correlated to the film’s macrostrain. TH microscopy presents a relatively simple all-optical method to monitor nanoscale anisotropy in thin films during exposure to high-intensity radiation and during deposition.

[1]  Michel Orrit,et al.  Third-harmonic generation from single gold nanoparticles. , 2005, Nano letters.

[2]  Yaron Silberberg,et al.  Depth-resolved multiphoton polarization microscopy by third-harmonic generation. , 2003, Optics letters.

[3]  J. Squier,et al.  Determination of material properties by use of third-harmonic generation microscopy. , 2002 .

[4]  Dan Oron,et al.  Background-free third harmonic imaging of gold nanorods. , 2009, Nano letters.

[5]  W. K. Burns,et al.  Third-Harmonic Generation in Absorbing Media of Cubic or Isotropic Symmetry , 1971 .

[6]  J. Yguerabide,et al.  Light-scattering submicroscopic particles as highly fluorescent analogs and their use as tracer labels in clinical and biological applications. , 1998, Analytical biochemistry.

[7]  S. V. Fomichev,et al.  Laser-induced nonlinear excitation of collective electron motion in a cluster , 2003 .

[8]  Yaron Silberberg,et al.  Multiphoton plasmon-resonance microscopy. , 2003, Optics express.

[9]  K R Wilson,et al.  Third harmonic generation microscopy. , 1998, Optics express.

[10]  J. Yguerabide,et al.  Light-scattering submicroscopic particles as highly fluorescent analogs and their use as tracer labels in clinical and biological applications. , 1998, Analytical biochemistry.

[11]  Yaron Silberberg,et al.  Depth-resolved structural imaging by third-harmonic generation microscopy. , 2004, Journal of structural biology.

[12]  Roger Route,et al.  Advances in ion beam sputtered Sc2O3 for optical interference coatings , 2010, Laser Damage.

[13]  T. Masuda,et al.  Ultra-high residual compressive stress (>2 GPa) in a very small volume (<1 μm3) of indented quartz , 2011 .

[14]  Luke A. Emmert,et al.  Modeling the effect of native and laser-induced states on the dielectric breakdown of wide band gap optical materials by multiple subpicosecond laser pulses , 2010 .

[15]  D Yelin,et al.  Laser scanning third-harmonic-generation microscopy in biology. , 1999, Optics express.

[16]  Vladislav V. Yakovlev,et al.  Diagnostics of surface layer disordering using optical third harmonic generation of a circular polarized light , 2001 .