All-Optical Patterning of Au Nanoparticles on Surfaces Using Optical Traps

Nano Letters ◽  
2010 ◽  
Vol 10 (11) ◽  
pp. 4302-4308 ◽  
Author(s):  
Mason J. Guffey ◽  
Norbert F. Scherer
2019 ◽  
Vol 512 ◽  
pp. 112-131 ◽  
Author(s):  
Volodymyr M. Kryshenik ◽  
Yuriy M. Azhniuk ◽  
Victor S. Kovtunenko

2010 ◽  
Vol 23 (6) ◽  
pp. 757-764 ◽  
Author(s):  
Oksana V. Sakhono ◽  
Joachim Stumpe ◽  
Leonid M. Goldenberg ◽  
Tatiana N. Smirnova ◽  
Lyudmila M. Kokhtych

Polymers ◽  
2020 ◽  
Vol 12 (9) ◽  
pp. 1960 ◽  
Author(s):  
Yue Cao ◽  
Daming Zhang ◽  
Yue Yang ◽  
Baizhu Lin ◽  
Jiawen Lv ◽  
...  

This article demonstrated the Au nanoparticles-doped polymer all-optical switches based on photothermal effects. The Au nanoparticles have a strong photothermal effect, which would generate the inhomogeneous thermal field distributions in the waveguide under the laser irradiation. Meanwhile, the polymer materials have the characteristics of good compatibility with photothermal materials, low cost, high thermo-optical coefficient and flexibility. Therefore, the Au nanoparticles-doped polymer material can be applied in optically controlled optical switches with low power consumption, small device dimension and high integration. Moreover, the end-pumping method has a higher optical excitation efficiency, which can further reduce the power consumption of the device. Two kinds of all-optical switching devices have been designed including a base mode switch and a first-order mode switch. For the base mode switch, the power consumption and the rise/fall time were 2.05 mW and 17.3/106.9 μs, respectively at the wavelength of 650 nm. For the first-order mode switch, the power consumption and the rise/fall time were 0.5 mW and 10.2/74.9 μs, respectively at the wavelength of 532 nm. This all-optical switching device has the potential applications in all-optical networks, flexibility device and wearable technology fields.


2001 ◽  
Vol 5 (6) ◽  
pp. 487-494 ◽  
Author(s):  
Kevin G. Yager ◽  
Christopher J. Barrett

Author(s):  
R. Hegerl ◽  
A. Feltynowski ◽  
B. Grill

Till now correlation functions have been used in electron microscopy for two purposes: a) to find the common origin of two micrographs representing the same object, b) to check the optical parameters e. g. the focus. There is a third possibility of application, if all optical parameters are constant during a series of exposures. In this case all differences between the micrographs can only be caused by different noise distributions and by modifications of the object induced by radiation.Because of the electron noise, a discrete bright field image can be considered as a stochastic series Pm,where i denotes the number of the image and m (m = 1,.., M) the image element. Assuming a stable object, the expectation value of Pm would be Ηm for all images. The electron noise can be introduced by addition of stationary, mutual independent random variables nm with zero expectation and the variance. It is possible to treat the modifications of the object as a noise, too.


1988 ◽  
Vol 49 (C2) ◽  
pp. C2-459-C2-462 ◽  
Author(s):  
F. A.P. TOOLEY ◽  
B. S. WHERRETT ◽  
N. C. CRAFT ◽  
M. R. TAGHIZADEH ◽  
J. F. SNOWDON ◽  
...  
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