Abstract
The optical second-harmonic response of a finite hexagonal lattice is computed as a function of the inter particle separation. In agreement with experiments on Langmuir monolayers of silver quantum dots, the computed response exhibits a peak due to a transition from localized electronic states to a band-like structure. The localization is due to the fluctuations in the particle size and position. For a perfect lattice the variation of the nonlinear response with the inter particle separation is qualitatively different. The role of the symmetry breaking is demonstrated at the tight binding level of electronic structure computations.
Original language | English |
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Pages (from-to) | 453-458 |
Number of pages | 6 |
Journal | Chemical Physics Letters |
Volume | 291 |
Issue number | 3-4 |
DOIs | |
State | Published - Jul 17 1998 |
Externally published | Yes |
Funding
We thank Professor S. Efrima for discussions. FR is Chercheur Qualifié, FNRS, Belgium. This work was partly supported by the James Franck program (FR and RDL) and NSF-National Young Investigator program and ONR order N00014-95-F-0099 (JRH) and used the computational facilities of UCLA and of SFB 377.
Funders | Funder number |
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NSF-National | |
Office of Naval Research | N00014-95-F-0099 |
University of California, Los Angeles | SFB 377 |