Measurement of the nonlinear refractive index of air constituents at mid-infrared wavelengths.

We measure the nonlinear refractive index coefficients in N₂, O₂, and Ar from visible through mid-infrared wavelengths (λ=0.4-2.4  μm). The wavelengths investigated correspond to transparency windows in the atmosphere. Good agreement is found with theoretical models of χ((3)). Our results are essential for accurately simulating the propagation of ultrashort mid-infrared pulses in the atmosphere.

[1]  David P. Shelton,et al.  Measurements and calculations of the hyperpolarizabilities of atoms and small molecules in the gas phase , 1994 .

[2]  D. M. Bishop General dispersion formulas for molecular third‐order nonlinear optical properties , 1989 .

[3]  M. Spackman Time‐dependent Hartree–Fock second‐order molecular properties with a moderately sized basis set. I. The frequency dependence of the dipole polarizability , 1991 .

[4]  O. Faucher,et al.  Measurement of high order Kerr refractive index of major air components. , 2009, Optics express.

[5]  Direct imaging of the acoustic waves generated by femtosecond filaments in air. , 2014, Optics letters.

[6]  Thomas M. Antonsen,et al.  Simulations of femtosecond atmospheric filaments enhanced by dual pulse molecular alignment , 2012 .

[7]  S. Skupin,et al.  Ultrashort filaments of light in weakly ionized, optically transparent media , 2007 .

[8]  Peng Zhao,et al.  Beam deflection measurement of bound-electronic and rotational nonlinear refraction in molecular gases. , 2015, Optics express.

[9]  H. Milchberg,et al.  Subject Areas : Optics A Viewpoint on : Demonstration of Long-Lived High-Power Optical Waveguides in Air , 2014 .

[10]  S. Zahedpour,et al.  Sensitivity of propagation and energy deposition in femtosecond filamentation to the nonlinear refractive index , 2014, 1411.4914.

[11]  Single-shot supercontinuum spectral interferometry , 2002 .

[12]  George Rodriguez,et al.  Coherent control of terahertz supercontinuum generation in ultrafast laser–gas interactions , 2008 .

[13]  Shelton Nonlinear-optical susceptibilities of gases measured at 1064 and 1319 nm. , 1990, Physical review. A, Atomic, molecular, and optical physics.

[14]  Mordechai Segev,et al.  Long-Lived Waveguides and Sound Wave Generation by Laser Filamentation , 2013, 1307.3588.

[15]  Richard L. Sutherland,et al.  Handbook of Nonlinear Optics , 1996 .

[16]  Zach DeVito,et al.  Opt , 2017 .

[17]  Alan K. Burnham,et al.  Measurement of the dispersion in polarizability anisotropies , 1975 .

[18]  A. Mysyrowicz,et al.  Self-seeded lasing in ionized air pumped by 800 nm femtosecond laser pulses. , 2013, Optics express.

[19]  H. Milchberg,et al.  Optical mode structure of the air waveguide. , 2014, Optics letters.

[20]  Miroslav Kolesik,et al.  Super high power mid-infrared femtosecond light bullet , 2015, Nature Photonics.

[21]  Y.-H. Cheng,et al.  Absolute measurement of the transient optical nonlinearity in N 2 , O 2 , N 2 O, and Ar , 2012 .

[22]  S. Alisauskas,et al.  Remotely pumped stimulated emission at 337 nm in atmospheric nitrogen , 2013, 2013 Conference on Lasers & Electro-Optics Europe & International Quantum Electronics Conference CLEO EUROPE/IQEC.

[23]  A. Voronin,et al.  Mid-infrared laser filamentation in molecular gases. , 2013, Optics letters.

[24]  J. Rice Frequency‐dependent hyperpolarizabilities for argon, krypton, and neon: Comparison with experiment , 1992 .

[25]  J. Moloney,et al.  Modeling and simulation techniques in extreme nonlinear optics of gaseous and condensed media , 2014, Reports on progress in physics. Physical Society.

[26]  N. Jhajj,et al.  The effect of long timescale gas dynamics on femtosecond filamentation , 2013, CLEO: 2013.

[27]  H. Milchberg,et al.  Collection of remote optical signals by air waveguides , 2014, 2014 Conference on Lasers and Electro-Optics (CLEO) - Laser Science to Photonic Applications.

[28]  R. Bartlett,et al.  Hyperpolarizabilities of molecules with frequency dependence and electron correlation , 1991 .

[29]  H. Milchberg,et al.  Single-shot, space- and time-resolved measurement of rotational wavepacket revivals in H(2), D(2), N(2), O(2), and N(2)O. , 2007, Optics express.

[30]  A. Couairon,et al.  Modeling the filamentation of ultra-short pulses in ionizing media , 2000 .

[31]  A. T. Tokunaga,et al.  The Mauna Kea Observatories Near‐Infrared Filter Set. I. Defining Optimal 1–5 Micron Bandpasses , 2002 .

[32]  M. Murnane,et al.  Bright Coherent Ultrahigh Harmonics in the keV X-ray Regime from Mid-Infrared Femtosecond Lasers , 2012, Science.

[33]  M. Scully,et al.  High-Gain Backward Lasing in Air , 2010, Science.

[34]  U. Morgner,et al.  Low- and high-order harmonic generation inside an air filament , 2012 .

[35]  A. Couairon,et al.  Femtosecond filamentation in transparent media , 2007 .

[36]  Optical beam dynamics in a gas repetitively heated by femtosecond filaments. , 2013, Optics express.