Resonant Exciton Second-harmonic Generation in Self-assembled ZnO Microcrystallite Thin Films

Second-harmonic generation has been studied for fundamental wavelengths from 720 to 1100 nm on high-quality ZnO thin films deposited on sapphire substrates by laser molecular beam epitaxy. The second-order nonlinear susceptibility components increase dramatically as the second-harmonic frequency approaches the ZnO bandgap. The increase is most likely due to a resonance of the second-harmonic frequency with the critical point transition associated with the direct bandgap transition. Large second-order nonlinear susceptibility components were determined to have a nonresonant background value of −83.7 pm V−1 for d33, 14.7 pm V−1 for d31 and 15.2 pm V−1 for d15 for a fundamental wavelength of 1064 nm. The value of d33 for the film was as high as 14 times that of bulk material in the nonresonant region. The difference in values between the second nonlinear coefficients of the bulk and the film may originate from the microcrystallite structure.

[1]  Eric Dumont,et al.  Simultaneous determination of the optical properties and of the structure of r.f.-sputtered ZnO thin films , 1999 .

[2]  Robert P. H. Chang,et al.  Second harmonic generation in laser ablated zinc oxide thin films , 1998 .

[3]  Masashi Kawasaki,et al.  Room-temperature ultraviolet laser emission from self-assembled ZnO microcrystallite thin films , 1998 .

[4]  Juh Tzeng Lue,et al.  Optical second harmonic generation from thin silver films , 1997 .

[5]  Shuji Nakamura,et al.  SUBBAND EMISSIONS OF INGAN MULTI-QUANTUM-WELL LASER DIODES UNDER ROOM-TEMPERATURE CONTINUOUS WAVE OPERATION , 1997 .

[6]  D. Blanc,et al.  All-optical probing of material structure by second-harmonic generation: application to piezoelectric aluminum nitride thin films , 1997 .

[7]  L. Pfeiffer,et al.  Gain Spectra and Stimulated Emission in Epitaxial (In,Al) GaN Thin Films , 1996 .

[8]  Shuji Nakamura,et al.  Ridge‐geometry InGaN multi‐quantum‐well‐structure laser diodes , 1996 .

[9]  B. Mendoza,et al.  Model for great enhancement of second-harmonic generation in quantum dots , 1995 .

[10]  Mark A. Ratner,et al.  Dispersion of second‐order optical nonlinearity in chromophoric self‐assembled films by optical parametric amplification: Experiment and theory , 1994 .

[11]  J. Coutaz,et al.  Characterization of aluminium nitride thin film structure using second-harmonic generation , 1994 .

[12]  H. Koinuma,et al.  Controlled formation of oxide materials by laser molecular beam epitaxy , 1994 .

[13]  P. Lundquist,et al.  Second order optical nonlinearities of radio frequency sputter‐deposited AlN thin films , 1993 .

[14]  W. Richter,et al.  Low temperature MOVPE growth of ZnSe with ditertiarybutylselenide , 1992 .

[15]  Mengyan Shen,et al.  Optically pumped lasing of ZnO at room temperature , 1991 .

[16]  Yaochun Shen,et al.  High-power, widely tunable, picosecond coherent source from optical parametric amplification in barium borate , 1990 .

[17]  G. Koren,et al.  Dispersion of nonlinear optical susceptibility in GaAs and GaSb , 1974 .

[18]  D. Haueisen,et al.  Resonant Second-Harmonic Generation in the Exciton Region of CuCl and ZnO , 1973 .

[19]  Robert C. Miller,et al.  Absolute signs of nonlinear optical coefficients of polar crystals , 1970 .

[20]  N. Bloembergen,et al.  Measurement of the Lowest-Order Nonlinear Susceptibility in III—V Semiconductors by Second-Harmonic Generation with a CO2Laser , 1969 .

[21]  C. Tuttle The relation between diffuse and specular density , 1926 .