Strong Wavelength Dependence of Hyperpolarizability in the Near-Infrared Biological Window for Second-Harmonic Generation by Amphiphilic Porphyrins

We have applied the Thomas-Kuhn sum rules to model the wavelength dependence of the second-order nonlinear polarizability of an amphiphilic porphyrin chromophore designed for cellular imaging on the basis of the complete analysis of its linear absorption spectrum. We predict huge oscillations for this first hyperpolarizability in the biological transparency window with the second-order response exhibiting three minima and two maxima in the wavelength range between 700 and 900 nm and a second region of enhanced response between 1200 and 1500 nm. We confirmed the predicted values experimentally demonstrating both the validity of our approach and the need for a wavelength scan to find a maximum in the resonance-enhanced signal for cellular imaging. These results suggest a new approach toward achieving spectroscopic selectivity during second-harmonic generation imaging.

[1]  K. Wostyn,et al.  High-frequency demodulation of multiphoton fluorescence in long-wavelength hyper-Rayleigh scattering. , 1999, Optics letters.

[2]  Leslie M Loew,et al.  Second-harmonic imaging microscopy for visualizing biomolecular arrays in cells, tissues and organisms , 2003, Nature Biotechnology.

[3]  Mark G. Kuzyk,et al.  Experimental verification of a self-consistent theory of the first-, second-, and third-order (non)linear optical response , 2009, 0908.3203.

[4]  Mark G. Kuzyk,et al.  Why do we need three levels to understand the molecular optical response? , 2011, Organic Photonics + Electronics.

[5]  Kuzyk Physical limits on electronic nonlinear molecular susceptibilities , 2000, Physical review letters.

[6]  Koen Clays,et al.  Why hyperpolarizabilities fall short of the fundamental quantum limits. , 2004, The Journal of chemical physics.

[7]  Mark G. Kuzyk,et al.  Nonlinear Optics: Fundamental Limits ofNonlinear Susceptibilities , 2003 .

[8]  Koen Clays,et al.  Hyper-Rayleigh scattering in the Fourier domain for higher precision: Correcting for multiphoton fluorescence with demodulation and phase data , 2001 .

[9]  Mark G. Kuzyk,et al.  Erratum: “Why hyperpolarizabilities fall short of the fundamental quantum limit” [J. Chem. Phys.121, 7932 (2004)] , 2006 .

[10]  Javier Perez-Moreno,et al.  Theoretical and experimental characterization of the first hyperpolarizability , 2007 .

[11]  Persoons,et al.  Hyper-Rayleigh scattering in solution. , 1991, Physical review letters.

[12]  Brian J. Orr,et al.  Perturbation theory of the non-linear optical polarization of an isolated system , 1971 .

[13]  Joseph T. Hupp,et al.  Electronic Stark Effect Studies of a Porphyrin-Based Push−Pull Chromophore Displaying a Large First Hyperpolarizability: State-Specific Contributions to β , 1998 .

[14]  Mark G. Kuzyk,et al.  Fundamental limits on third-order molecular susceptibilities: erratum , 2003 .

[15]  Koen Clays,et al.  High-frequency demodulation of multi-photon fluorescence in hyper-Rayleigh scattering , 1998 .

[16]  Koen Clays,et al.  Molecular engineering of chromophores for combined second-harmonic and two-photon fluorescence in cellular imaging , 2012 .

[17]  Koen Clays,et al.  Amphiphilic porphyrins for second harmonic generation imaging. , 2009, Journal of the American Chemical Society.

[18]  Inge Asselberghs,et al.  Unusual frequency dispersion effects of the nonlinear optical response in highly conjugated (polypyridyl)metal-(porphinato)zinc(II) chromophores. , 2002, Journal of the American Chemical Society.

[19]  Koen Clays,et al.  Dyes for biological second harmonic generation imaging. , 2010, Physical chemistry chemical physics : PCCP.

[20]  J. Oudar,et al.  Hyperpolarizabilities of the nitroanilines and their relations to the excited state dipole moment , 1977 .

[21]  Inge Asselberghs,et al.  Predicting the Frequency Dispersion of Electronic Hyperpolarizabilities on the Basis of Absorption Data and Thomas−Kuhn Sum Rules , 2010 .

[22]  Masahiro Ito,et al.  Ex vivo and in vivo second-harmonic-generation imaging of dermal collagen fiber in skin: comparison of imaging characteristics between mode-locked Cr:forsterite and Ti:sapphire lasers. , 2009, Applied optics.

[23]  Michael J. Therien,et al.  Physical chemistry: How to improve your image , 2009, Nature.