1998
DOI: 10.1364/josab.15.000257
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Multipolar molecules and multipolar fields: probing and controlling the tensorial nature of nonlinear molecular media

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Cited by 271 publications
(222 citation statements)
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“…[16][17][18][19][20][21][22][23][24]. The starting point is a consideration of the irreducible Cartesian tensor components of the polarization and molecular response tensors [13].…”
Section: Symmetry-based Selection Rulesmentioning
confidence: 99%
“…[16][17][18][19][20][21][22][23][24]. The starting point is a consideration of the irreducible Cartesian tensor components of the polarization and molecular response tensors [13].…”
Section: Symmetry-based Selection Rulesmentioning
confidence: 99%
“…Since the chromophores are polar molecules with a static dipole moment μ 0 , they will interact, thereby minimizing their energy and forming an anti-ferroelectric state, where neighbouring chromophores are preferentially oriented in opposite directions, leading to a decrease of the effective electro-optic coefficient [27]. In order to avoid the negative interaction between chromophores, non-polar second order nonlinear molecule were proposed [35]. Unfortunately, in these molecules, since they have no μ 0 , it is not possible to align them using the standard poling procedure shown previously.…”
Section: Steady-state Properties Of the Induced Electo-optic Coefficientmentioning
confidence: 99%
“…Unfortunately, in these molecules, since they have no μ 0 , it is not possible to align them using the standard poling procedure shown previously. A more complicated all-optical poling was proposed [35].…”
Section: Steady-state Properties Of the Induced Electo-optic Coefficientmentioning
confidence: 99%
“…The result accommodates both near-field and wave-zone limits. In the near-field; when kR  1, virtual features of the emergent photon are most apparent, [27] and the electric field has significant longitudinal components with respect to R; transversality emerges with propagation into the wave-zone, kR  1, as forward propagation becomes dominated by contributions with wave-vector k closely parallel to R. Moreover, the index-symmetric tensor V can be cast as a sum of two terms, one associated with angular momentum j = 0, the other j = 2, respectively represented by the two squarebracketed terms on the right in the following; [30][31][32] ( ) ( ) …”
Section: Fi R I F S I F T I F I T I S I R F H T T H R S H R R H I M Ementioning
confidence: 99%