Dynamical calculation of third harmonic generation in a semiconductor quantum well

Nonlinear phenomena in optically excited semiconductor structures are of high interest. Here we develop a model capable of studying the dynamics of the photoexcited carriers, including Coulomb interaction on a Hartree-Fock level, on the same footing as the dynamics of the light field impinging on an arbitrary photonic structure. Applying this method to calculate the third-harmonic generation in a semiconductor quantum well embedded in a Bragg mirror structure, we find that the power-law exponent of the intensity dependence of the third-harmonic generation depends on the frequency of the exciting pulse. Off-resonant pulses follow the expected cubic dependence, while the exponent is smaller for resonant pulses due to saturation effects in the induced carrier density. Our study provides a detailed understanding of the carrier and light field dynamics during nonlinear processes.

[1]  M. Wegener,et al.  Signatures of carrier-wave Rabi flopping in GaAs. , 2001, Physical review letters.

[2]  T. Kuhn,et al.  Controlling the capture dynamics of traveling wave packets into a quantum dot , 2006 .

[3]  Fausto Rossi,et al.  Theory of ultrafast phenomena in photoexcited semiconductors , 2002 .

[4]  U. Peschel,et al.  Light-matter interaction and lasing in semiconductor nanowires: A combined finite-difference time-domain and semiconductor Bloch equation approach , 2014, 1410.4670.

[5]  Koch,et al.  Rabi flopping in semiconductors. , 1994, Physical review letters.

[6]  I. Al-Naib,et al.  High harmonic generation in undoped graphene: Interplay of inter- and intraband dynamics , 2014, 1407.1273.

[7]  F. Rossi,et al.  Microscopic modeling of scattering quantum non-locality in semiconductor nanostructures , 2013 .

[8]  Y. Wang,et al.  Single-mode laser by parity-time symmetry breaking , 2014, Science.

[9]  Ziółkowski,et al.  Ultrafast pulse interactions with two-level atoms. , 1995, Physical review. A, Atomic, molecular, and optical physics.

[10]  Costas M. Soukoulis,et al.  Self-consistent calculations of loss-compensated fishnet metamaterials , 2010, 1008.4956.

[11]  Nasser N Peyghambarian,et al.  Direct observation of excitonic rabi oscillations in semiconductors , 1999 .

[12]  J. Sipe,et al.  Numerical study of the optical nonlinearity of doped and gapped graphene: From weak to strong field excitation , 2015, 1509.01209.

[13]  Leroy L. Chang,et al.  Exciton binding energy in quantum wells , 1982 .

[14]  Ortwin Hess,et al.  Cavity-free plasmonic nanolasing enabled by dispersionless stopped light , 2014, Nature Communications.

[15]  A. Lisyansky,et al.  Self-consistent Hartree method for calculations of exciton binding energy in quantum wells , 2006 .

[16]  Ortwin Hess,et al.  Gain and plasmon dynamics in active negative-index metamaterials , 2010, Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[17]  Andreas Pusch,et al.  Control and dynamic competition of bright and dark lasing states in active nanoplasmonic metamaterials , 2011, 1112.4367.

[18]  Ingolf V. Hertel,et al.  Experimental and theoretical study of third-order harmonic generation in carbon nanotubes , 2002 .

[19]  J. Dadap,et al.  Optical Third-Harmonic Generation in Graphene , 2013, 1301.1697.

[20]  Guang-hui Wang Third-harmonic generation in cylindrical parabolic quantum wires with an applied electric field , 2005 .

[21]  Intensity dependence of signals obtained in four-wave-mixing geometry : influence of higher-order contributions , 2000 .

[22]  Ortwin Hess,et al.  A full-time-domain approach to spatio-temporal dynamics of semiconductor lasers. I. Theoretical formulation , 2008 .

[23]  Ortwin Hess,et al.  A full time-domain approach to spatio-temporal dynamics of semiconductor lasers. II. Spatio-temporal dynamics , 2008 .

[24]  Ortwin Hess,et al.  Overcoming losses with gain in a negative refractive index metamaterial. , 2010, Physical review letters.

[25]  Gert-Jan Bakker,et al.  Third harmonic generation microscopy of cells and tissue organization , 2016, Journal of Cell Science.

[26]  Hopkins,et al.  Resonant harmonic generation and dynamic screening in a double quantum well. , 1994, Physical review letters.

[27]  G. Slepyan,et al.  Third-order optical nonlinearity in single-wall carbon nanotubes , 2006 .

[28]  Hartmut Haug,et al.  Ultrafast Quantum Kinetics of Time-Dependent RPA-Screened Coulomb Scattering , 1998 .

[29]  Hui Zhao,et al.  Third-harmonic generation in ultrathin films of MoS2. , 2014, ACS applied materials & interfaces.

[30]  Chi‐Kuang Sun,et al.  Third-harmonic generation microscopy reveals dental anatomy in ancient fossils. , 2015, Optics letters.

[31]  Trinesha Mosely,et al.  Third harmonic generation in a Quantum Cascade laser with monolithically integrated resonant optical nonlinearity. , 2004, Optics express.

[32]  Cho,et al.  Giant, triply resonant, third-order nonlinear susceptibility chi 3 omega (3) in coupled quantum wells. , 1992, Physical review letters.

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

[34]  O. Hess,et al.  Controllable interaction of counterpropagating solitons in three-level media , 2010 .