Compression Induced Chirality in Dense Molecular Films at the Air−Water Interface Probed by Second Harmonic Generation

Surface second harmonic generation was used to study the nonlinear optical properties of a two-dimensional film of 4-(4-(dihexadecylamino)styryl)-N-methylpyridinium iodide (DiA) formed at the air−water interface in a Langmuir trough. The second harmonic intensity was measured as a function of the incident fundamental and outgoing harmonic wave polarization angles during the monolayer compression. Below a critical average density of 0.55 nmol/cm2, the film is in a liquid-expanded state and the DiA molecules are strongly tilted on the interface. Above this critical average surface density, the film reveals chirality arising from the formation of molecular aggregates at the interface. It is demonstrated through a full analysis of the data that the origin of this chiral property of the film arises from the coupling of the electric and magnetic fields at the fundamental frequency.

[1]  Ude Scheunemann,et al.  Second-harmonic generation in Langmuir–Blodgett monolayers of stilbazium salt and phenylhydrazone dyes , 1988 .

[2]  Janice M. Hicks,et al.  Circular dichroism spectroscopy at interfaces: a surface second harmonic generation study , 1993 .

[3]  P. Bohn,et al.  Electronic resonance and local field effects on the nonlinear optical activity of H-aggregate-forming stilbazolium amphiphiles , 1995 .

[4]  M. Schanne-Klein,et al.  Application of classical models of chirality to surface second harmonic generation , 2001 .

[5]  Pierre F. Brevet Phenomenological three-layer model for surface second-harmonic generation at the interface between two centrosymmetric media , 1996 .

[6]  H. Watarai,et al.  Non-linear optical activity of porphyrin aggregate at the liquid/liquid interface , 2004 .

[7]  Thierry Boulesteix,et al.  Chiroptical effects in the second harmonic signal of collagens I and IV. , 2005, Journal of the American Chemical Society.

[8]  A. Persoons,et al.  Linearly and Circularly Polarized Probes of Second-Order Optical Activity of Chiral Surfaces , 1996, Organic Thin Films for Photonic Applications.

[9]  André Persoons,et al.  Second-order nonlinear optical properties of chiral materials , 2003 .

[10]  P. Pershan NONLINEAR OPTICAL PROPERTIES OF SOLIDS: ENERGY CONSIDERATIONS , 1963 .

[11]  Peterson,et al.  Chiral and herringbone symmetry breaking in water-surface monolayers. , 1996, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[12]  Jeffery J. Maki,et al.  Linearly polarized probes of surface chirality , 1995 .

[13]  Jing Yuan,et al.  Chiral molecular assemblies from a novel achiral amphiphilic 2-(heptadecyl) naphtha[2,3]imidazole through interfacial coordination. , 2003, Journal of the American Chemical Society.

[14]  J. Zasadzinski,et al.  Spontaneous chiral symmetry breaking by achiral molecules in a Langmuir–Blodgett film , 1994, Nature.

[15]  O. Tillement,et al.  Correlation reflectance spectroscopy of heterogeneous silver nanoparticle films upon compression at the air/water interface , 2008 .

[16]  François Hache,et al.  Off resonance second order optical activity of isotropic layers of chiral molecules: Observation of electric and magnetic contributions , 1998 .

[17]  Jeffery J. Maki,et al.  One‐electron second‐order optical activity of a helix , 1996 .

[18]  P. Bohn,et al.  Characterization of an aggregate-sensitive single-component energy-transfer system , 1993 .

[19]  M. Liu,et al.  Fabrication of Chiral Langmuir−Schaefer Films from Achiral TPPS and Amphiphiles through the Adsorption at the Air/Water Interface , 2003 .

[20]  François Hache,et al.  Nonlinear optical spectroscopy of chiral molecules. , 2005, Chirality.

[21]  J. Byers,et al.  A second harmonic generation analog of optical rotatory dispersion for the study of chiral monolayers , 1994 .

[22]  Maki,et al.  Surface second-harmonic generation from chiral materials. , 1995, Physical review. B, Condensed matter.

[23]  J. Byers,et al.  Consequences of chirality in second-order non-linear spectroscopy at surfaces. , 1994, Faraday discussions.

[24]  E. Adler,et al.  Nonlinear Optical Frequency Polarization in a Dielectric , 1964 .

[25]  Goldmann,et al.  Spontaneous chiral segregation in bidimensional films. , 1995, Physical review letters.

[26]  G. Wegner,et al.  Amphiphilic dyes for nonlinear optics: Dependence of second harmonic generation on functional group substitution† , 1991 .

[27]  Jeffery J. Maki,et al.  Second‐harmonic generation from chiral surfaces , 1994 .

[28]  Daniel A. Higgins,et al.  Optical second harmonic generation as a probe of surface chemistry , 1994 .