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Oriented crystallization of NLO organic materials
Affiliation:1. Université de Mons-Hainaut, Laboratoire de PhysicoChimie des Polymères, 20, Place du Parc, B-7000 Mons, Belgium;2. Ecole Normale Supérieure de Cachan, Laboratoire de Photonique Quantique et Moléculaire (UMR CNRS #8537) 61, Avenue Président Wilson, 94235 Cachan Cedex, France;1. Department of Physics, University of Lucknow, 226007 Lucknow, India;2. Group of Computational and Pharmaceutical Chemistry, LMCE Laboratory, Faculty of Sciences, University of Biskra, 07000 Biskra, Algeria;1. Department of Physics, Sriram Engineering College, Perumalpattu, Thiruvallur District 602024, India;2. Department of Physics, Prathyusha Institute of Technology and Management, Thiruvallur District 602025, India;3. Department of Physics, Government Arts College, Chennai 600005, India;1. Center for Nanosafety Metrology, Korea Research Institute of Standards and Science, Daejeon, Republic of Korea;2. Department of Nanobio Surface Science, Korea University of Science and Technology, Daejeon, Republic of Korea;3. Center for Energy Materials Metrology, Korea Research Institute of Standards and Science, Daejeon, Republic of Korea;4. Department of Mechanical Engineering, Korea University, Seoul, Republic of Korea;5. Department of New Biology, Daegu Gyeongbuk Institute of Science and Technology, Daegu, Republic of Korea;1. Research & Development centre, Bharathiar university, Coimbatore, Tamil Nadu, India;2. Post-Graduate and Research Department of Chemistry, Sri. Ramakrishna Mission Vidyalaya College of Arts and Science, Coimbatore, 641 020, Tamil Nadu, India;3. Pachamuthu college of Arts and Science for Women, Dharmapuri 636 705, Tamil Nadu, India;4. Dr. N.G.P. Institute of Technology, Coimbatore 641048, Tamil Nadu, India
Abstract:A new methodology to study the second order NLO coefficients of organic materials was developed. We have demonstrated that the combination of oriented crystal growth on structured surfaces, grazing incidence X-ray diffraction and second harmonic ellipsometry gives an insight of the relations between the molecular hyperpolarizability and the crystalline non-linear susceptibility tensor. Thin organic layers of 2-methyl-4-nitroaniline (MNA), N-(4-nitrophenyl)-l-prolinol (NPP) and 2-(N,N-dimethylamino)-5-nitroacetanilide (DAN) were grown on poly(tetrafluoroethylene) (PTFE) substrates prepared by the friction transfer method. From the observed crystallographic orientations, a growth mechanism based on a “soft-epitaxy” was proposed. At low substrate temperature, the overlayer-substrate interactions dominate and induce a two-dimensional epitaxial growth which corresponds to a specific physisorption of aromatic molecules on the polymer surface. At high substrate temperature, the aromatic crystals nucleate via a grapho-epitaxy mechanism which occurs on topological defects of the surface. The formation of specific interactions with the PTFE substrates is not a requisite to orient the crystals in this model. Finally, we will show that the ratio between the non-vanishing components of the first non-linear susceptibility tensor (χijk or dij) can be estimated from second harmonic ellipsometry measurements.
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