Transmission coefficients, relative modal powers and radiated field patterns in overmoded coaxial waveguides

2006 ◽  
Vol 153 (6) ◽  
pp. 222 ◽  
Author(s):  
J.G. Davis ◽  
A.A.P. Gibson
2011 ◽  
Vol 70 (13) ◽  
pp. 1121-1131
Author(s):  
V. S. Miroshnichenko ◽  
V. G. Dudka ◽  
D. V. Yudintsev

2021 ◽  
Vol 118 (13) ◽  
pp. 131105
Author(s):  
Oshri Rabinovich ◽  
Ariel Epstein
Keyword(s):  

2021 ◽  
Vol 129 (19) ◽  
pp. 193103
Author(s):  
Amirreza Mahigir ◽  
Georgios Veronis

2008 ◽  
Vol 41 (1) ◽  
pp. 18-26 ◽  
Author(s):  
Václav Holý ◽  
Paul F. Fewster

A new method is presented for a calculation of the reciprocal-space distribution of X-ray diffracted intensity along a crystal truncation rod. In contrast to usual kinematical or dynamical approaches, the method is correct both in the reciprocal-lattice points and between them. In the method, the crystal is divided into a sequence of very thin slabs parallel to the surface; in contrast to the well known Darwin dynamical theory, the electron density in the slabs is constant along the surface normal. The diffracted intensity is calculated by a matrix formalism based on the Fresnel reflection and transmission coefficients. The method is applicable for any polarization of the primary beam and also in a non-coplanar scattering geometry.


Nano Letters ◽  
2013 ◽  
Vol 13 (10) ◽  
pp. 4753-4758 ◽  
Author(s):  
Wonseok Shin ◽  
Wenshan Cai ◽  
Peter B. Catrysse ◽  
Georgios Veronis ◽  
Mark L. Brongersma ◽  
...  
Keyword(s):  

2021 ◽  
Vol 12 (1) ◽  
Author(s):  
Yongtao Liu ◽  
Zhiguang Zhou ◽  
Fan Wang ◽  
Günter Kewes ◽  
Shihui Wen ◽  
...  

AbstractSub-diffraction limited localization of fluorescent emitters is a key goal of microscopy imaging. Here, we report that single upconversion nanoparticles, containing multiple emission centres with random orientations, can generate a series of unique, bright and position-sensitive patterns in the spatial domain when placed on top of a mirror. Supported by our numerical simulation, we attribute this effect to the sum of each single emitter’s interference with its own mirror image. As a result, this configuration generates a series of sophisticated far-field point spread functions (PSFs), e.g. in Gaussian, doughnut and archery target shapes, strongly dependent on the phase difference between the emitter and its image. In this way, the axial locations of nanoparticles are transferred into far-field patterns. We demonstrate a real-time distance sensing technology with a localization accuracy of 2.8 nm, according to the atomic force microscope (AFM) characterization values, smaller than 1/350 of the excitation wavelength.


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