High-Optical-Quality Blends of Anionic Polymethine Salts and Polycarbonate with Enhanced Third-Order Non-linearities for Silicon-Organic Hybrid Devices

2012 ◽  
Vol 24 (44) ◽  
pp. OP326-OP330 ◽  
Author(s):  
Zhong'an Li ◽  
Yang Liu ◽  
Hyeongeu Kim ◽  
Joel M. Hales ◽  
Sei-Hum Jang ◽  
...  
2008 ◽  
Vol 20 (23) ◽  
pp. 4584-4587 ◽  
Author(s):  
Bweh Esembeson ◽  
Michelle L. Scimeca ◽  
Tsuyoshi Michinobu ◽  
François Diederich ◽  
Ivan Biaggio

Crystals ◽  
2021 ◽  
Vol 11 (5) ◽  
pp. 462
Author(s):  
Ji Xia ◽  
Fuyin Wang ◽  
Chunyan Cao ◽  
Zhengliang Hu ◽  
Heng Yang ◽  
...  

Optomechanical nanocavities open a new hybrid platform such that the interaction between an optical cavity and mechanical oscillator can be achieved on a nanophotonic scale. Owing to attractive advantages such as ultrasmall mass, high optical quality, small mode volume and flexible mechanics, a pair of coupled photonic crystal nanobeam (PCN) cavities are utilized in this paper to establish an optomechanical nanosystem, thus enabling strong optomechanical coupling effects. In coupled PCN cavities, one nanobeam with a mass meff~3 pg works as an in-plane movable mechanical oscillator at a fundamental frequency of . The other nanobeam couples light to excite optical fundamental supermodes at and 1554.464 nm with a larger than 4 × 104. Because of the optomechanical backaction arising from an optical force, abundant optomechanical phenomena in the unresolved sideband are observed in the movable nanobeam. Moreover, benefiting from the in-plane movement of the flexible nanobeam, we achieved a maximum displacement of the movable nanobeam as 1468 . These characteristics indicate that this optomechanical nanocavity is capable of ultrasensitive motion measurements.


2005 ◽  
Vol 86 (7) ◽  
pp. 071917 ◽  
Author(s):  
Y. D. Wang ◽  
S. J. Chua ◽  
S. Tripathy ◽  
M. S. Sander ◽  
P. Chen ◽  
...  

2021 ◽  
Author(s):  
Huajun Xu ◽  
Delwin L Elder ◽  
Lewis E Johnson ◽  
Wolfgang Heni ◽  
Yovan de Coene ◽  
...  

This study demonstrates enhancement of in-device electro-optic activity via a series of theory-inspired organic electro-optic (OEO) chromophores based on strong (diarylamino)phenyl electron donating moieties. These chromophores are tuned to minimize...


1989 ◽  
Vol 172 ◽  
Author(s):  
Mahmoud R. Shahriari ◽  
Tariq Iqbal ◽  
Paul R. Foy ◽  
Steve J. Saggese ◽  
G. H. Sigel

AbstractSeveral glass systems based on AIF3 have been synthesized and fabricated into preforms by controlled melting and rotational casting. High optical quality preforms have been drawn into fibers using a specially modified drawing facility. The drawing tower is enclosed with a vertical glove box in which the levels of both moisture and oxygen are kept below 1 ppm during the drawing. The AIF3 -based fibers have shown dramatically superior chemical durability relative to the ZrF4 -based glass fibers. Selected optical, mechanical and thermal properties of these fibers will be presented. AIF3 -based glass fibers offer interesting opportunities for short range applications in the 2–4 micron region of the infrared such as sensing, remote spectroscopy and laser power delivery.


2011 ◽  
Vol 99 (25) ◽  
pp. 251910 ◽  
Author(s):  
X. J. Chen ◽  
B. Gayral ◽  
D. Sam-Giao ◽  
C. Bougerol ◽  
C. Durand ◽  
...  

2010 ◽  
Vol 7 (7-8) ◽  
pp. 2079-2081 ◽  
Author(s):  
Dares Kaewket ◽  
Sakuntam Sanorpim ◽  
Sukkaneste Tungasmita ◽  
Ryuji Katayama ◽  
Kentaro Onabe

1989 ◽  
Vol 175 ◽  
Author(s):  
L. R. Dalton ◽  
L. P. Yu

AbstractSynthesis/processing schemes for the preparation of optical quality thin films of π-electron containing organic and organometallic materials are discussed. Fabrication approaches range from preparation of molecular/polymer composites, to preparation of copolymers containing pendant electroactive moieties, to preparation of copolymers with electroactive units incorporated into the polymer backbone, to the preparation of polymer/polymer composites. Such fabrication methodologies (particularly the latter three approaches) have the advantage of facilitating control over polymer solubility and of avoiding aggregation of electroactive units. The synthetic schemes discussed here yield materials with well-defined electroactive units; thus, diffuse bandedges associated with a distribution of π-electron conjugation lengths are avoided. Degenerate four wave mixing (DFWM) measurements at 532, 579–600, and 1064 nm are used to determine third order susceptibilities. Investigation of the frequency dependence of χ(3)/α established that resonance contributions dominate non-linear optical activity near the π-iπ* bandedge. A variety of electroactive moieties have been investigated with the largest values of χ(3)/α (= 10−12 esu cm) being observed for triphenodioxazine, metal phthalocyanine, metal tetraazaannulene, 6,6′-dimethoxy-quinolidine cyanine units.


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