Sci. <>/ProcSet[/PDF/Text/ImageB/ImageC/ImageI] >>/MediaBox[ 0 0 595.2 841.92] /Contents 4 0 R/Group<>/Tabs/S/StructParents 0>> From calculations treating the crystal as a sequence of planes that reproduces the observed average orientation, with each plane containing molecules ordered in a single orientation, the principal refractive indices at long wavelength (zero frequency) are estimated to be n1 = 1.500±0.01, n2 = 1.495±0.005, n3 = 1.420±0.005. 2000, 1 9 Introduction The electric moments of a molecule are quantities of fundamental importance in structural chemis- ... is the dipole moment … Access scientific knowledge from anywhere. Transition dipole moments of both Ph-substituted dimers correspond to an An localized transition (L a state) with the transition dipole along the An short molecular axis. © 2000 American Institute of Physics. Fluorescent probe made by (a) trapping growing polymer chain ends with a 9,10-substituted anthracene or by (b) polymerization initiated by a 9,10-substituted anthracene. ��Ֆ��U2]%����,�Fj�=�R%U��ԃЯ a�Ԑj�3R�!� �+@�A =�PC�A@�H5}=+ȱ[A�]=9v+ȱ[A�]=9�+ȱ_A�}=9�+ȱ_A�C=9+�qXA�C=9��kˢG�ҺW���J]W�"RC��� �H-="�0h�Dr��U6��]�EWߤh#�;�0I�X��8��(��Kw�Ѭ��y۴��٫�g��v]����X��7�1x���>k����E�`���q�.t�>��cjX�&�s�Q���n�lV΋E�,�� s6��x�_�iެ`�ع�-*��R�1�nt��d`~k�U� H/ue����hj��u��W7�Lmѡj�ڦ���V_͠k5h3tM[�lu��~�@@�Nz̫�5�,FT�j'�k��T6۵�vºVW[]]�R�Zˤ*ˎ�T �� ����,z�ʲ��Ԗ5��VKeg3�G_��6��V��Â�L��W�>�. If the symmetry of source and destination orbitals contributing to the electronic ... anthracene S1(π,π *) → S 0 8,500 5 x 10 7 5 x 10 7 0.4 9,10-diphenylanthracene S1(π,π *) → S 0 12,600 5 x 10 8 10 7 1.0 The zircon unit cell parameters calculated from XRD data of bulk powdered sample were: a=6.620(1); c=5.989(2). The results provide a key ingredient for theories of the optical and electrical properties of Langmuir–Blodgett films. General principles of the Ewald method for evaluating multipole lattice sums are reviewed. Problem 1. The results provide a basis for calculations of various surface-induced and surface-modified properties. This paper deals with the influence of a tuning capacitor on the relationship between the amplitude of the signal received by bulk wave electromagneto-acoustic transducers and the transducer-to-sample separation. For crystals of nonpolar molecules, the surface polarization is normally induced by incomplete cancellation of the electric fields of the molecular quadrupole moments; for crystals of polar molecules, it is produced by incomplete cancellation of the electric fields of the molecular dipole moments. Phys. Numerical calculations are presented in an accompanying paper. The higher the number of active frequencies in the IR of an organic molecule, the more asymmetric the molecule is [74]. <> Curved potential energy per molecule was drawn where it was adopted to change the length of the bonds (C 1-C 2),(C 1 = C 3)and(C 1-H 15) in the anthracene molecule compared to the result of values of total energy of anthracene in equilibrium situation. endobj J. Mol. Calculations for arbitrary planes are conveniently performed by transforming the conventional crystal unit cell to contain the desired plane as a face. The quadratic susceptibilities for surface SHG in anthracene and pyrene are roughly estimated as respectively 1/80 and 1/20 that in p-nitroaniline, reported to be 4 fm V−1; the coefficients could vary by one or two orders of magnitude among different surfaces. An electric dipole in an external electric field is subjected to a torque τ = p E sin θ, where θ is the angle between p and E . The first transition (S0→S1) occurs around 400 nm (3 eV) and has a transition dipole moment along the x direction. Anthracene and a chiral derivative of anthracene Athracene (see below) has two allowed optical transitions in the UV region of the spectrum. Algebraic treatments are developed for both cases, including all local‐field effects via planewise dipole sums. A brief discussion is given for absorption and reflection spectra, exciton band structure and exciton‐phonon coupling. The true values at optical frequencies should be larger and somewhat more anisotropic. Dipole Moment. But instead of focusing on those, I wanted to do another example which is an isomer of naphthalene. The present results provide input for calculations of surface-induced quadratic nonlinear optical response, reported in the following article. Phenanthrene occurs naturally and also is a man-made chemical. The surface has most effect on sums relating molecules in different surface layers. Algebraic results are obtained relating the local electric field and the macroscopic electric field in a surface layer to an applied uniform electric field, and hence to one another. Geometries were optimized at the HF/6-311G(3d,2p) level of theory. The treatment allows for the typically elongated shape of film-forming molecules. Using plane-waves and pseudo-potentials, as imple-mented in present codes, it is not possible to study truly isolated molecules or surfaces. Organic cocrystals exhibiting active optical waveguide behaviors are strongly related to the total internal reflection, molecule stacking modes, and the spatial distribution of transition dipole moment (µ) in crystals.However, organic charge transfer (CT) cocrystals as new materials that exhibit optical waveguide property responses to anisotropic spatial distribution of µ are still unknown. The effect of crystal symmetry on lattice sums is outlined; the number of independent sums relating different pairs of equivalent sublattices does not exceed the total number of such sublattices. Chem. The contribution from all plane sums not containing the origin is less than 10% of the total lattice sum for naphthalene, approximately 1% for anthracene and phenanthrene, and negligible in the cases of tetracene and pentacene. For each direction, two different terminations give different results. Some results for L axis dipoles on translationally inequivalent molecules are given below (units cm−1∕Å2). It arises from the molecular first hyperpolarizability, whether permanent or induced by electric fields at noncentrosymmetric sites in the bulk crystal or at sites in the surface region where centrosymmetry is lost. Detailed expressions are then derived for the surface second-harmonic generation in terms of the spatially varying molecular response and a microscopic expression that is derived for the variation of optical electric field through the surface region. Surface effects decrease sharply into the bulk, being negligible beyond neighboring layers of molecules. Dipole polarizabilities were calculated at the HF/6-311++G(3d,2p) and BLYP/6-311++G(3d,2p) levels of theory, using HF/6-311G(3d,2p) geometries. Previous theoretical results for surface linear optical response in molecular crystals are extended to treat response to the external applied field, the bulk macroscopic field, and the surface macroscopic field. molecular weight, moment of inertia, and dipole moment for molecule were calculated. The distribution of Pu in crystals is zoned and the Pu content varying from approximately 5 to 14 wt.% el. 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