Near-field effects on coherent anti-Stokes Raman scattering microscopy imaging.

We introduce a numerical method, the finite-difference time-domain (FDTD) method, to study the near-field effects on coherent anti-Stokes Raman Scattering (CARS) microscopy on nanoparticles. Changes of the induced nonlinear polarization, scattering patterns, and polarization properties against different diameters of spherical nanoparticles are calculated and discussed in details. The results show that due to near-field effects, the induced nonlinear polarization is significantly enhanced at the water-particle interface, with 1.5-fold increase in intensity compared to that inside the particles, and the near-field enhancement increases with decreasing diameters of nanoparticles. The enhanced scattering dominates over the scattering contribution from the particles when the nanoparticle size decreases down to the scale of less than a half wavelength of excitation light. Further studies show that near-field effects make the induced perpendicular polarization of CARS signals being strictly confined within the nanoparticles and the particle-water interface, and this perpendicular polarization component could contribute approximately 20% to the backward scattering. The ratio values of the perpendicular polarization component to the total CARS signals from nanoparticles sizing from 75 nm to 300 nm in backward scattering are approximately 3 to 5 times higher than those in forward scattering. Therefore, near-field effects can play an important role in CARS imaging. Employing the perpendicular polarization component of CARS signals can significantly improve the contrast of CARS images, and be particularly useful for revealing the fine structures of bio-materials with nano-scale resolutions.

[1]  Haim Lotem,et al.  Interference between Raman resonances in four-wave difference mixing , 1976 .

[2]  Esben Ravn Andresen,et al.  Broadband multiplex coherent anti-Stokes Raman scattering microscopy employing photonic-crystal fibers , 2005 .

[3]  S Y Hasegawa,et al.  Optical tunneling effect calculation of a solid immersion lens for use in optical disk memory. , 1999, Applied optics.

[4]  R. W. Terhune,et al.  Study of Optical Effects Due to an Induced Polarization Third Order in the Electric Field Strength , 1965 .

[5]  Antigoni Alexandrou,et al.  Fourier-transform coherent anti-Stokes Raman scattering microscopy. , 2006, Optics letters.

[6]  Yaron Silberberg,et al.  Single-pulse phase-contrast nonlinear Raman spectroscopy. , 2002, Physical review letters.

[7]  Andreas Volkmer,et al.  Theoretical and experimental characterization of coherent anti-Stokes Raman scattering microscopy , 2002 .

[8]  Riyi Shi,et al.  Coherent anti-stokes Raman scattering imaging of axonal myelin in live spinal tissues. , 2005, Biophysical journal.

[9]  Seung-Han Park,et al.  Anisotropy of near-field speckle patterns. , 2005, Optics letters.

[10]  K. Yee Numerical solution of initial boundary value problems involving maxwell's equations in isotropic media , 1966 .

[11]  Conor L Evans,et al.  Heterodyne coherent anti-Stokes Raman scattering (CARS) imaging. , 2006, Optics letters.

[12]  Ji-Xin Cheng,et al.  Green’s function formulation for third-harmonic generation microscopy , 2002 .

[13]  K. Takeda,et al.  Simultaneous measurement of size and refractive index of a fine particle in flowing liquid , 1992 .

[14]  T. WILSON,et al.  Finite sized coherent and incoherent detectors in confocal microscopy , 1996 .

[15]  E. Wolf,et al.  Electromagnetic diffraction in optical systems, II. Structure of the image field in an aplanatic system , 1959, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.