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Nanophotonics ◽  
2019 ◽  
Vol 8 (10) ◽  
pp. 1739-1745 ◽  
Author(s):  
Zhao Chen ◽  
Sai Chen ◽  
Yangyang Wang ◽  
Lin Xiao

AbstractChiral metamaterials provide a very convenient way to actively regulate the light field via external means, which is very important in nanophotonics. However, the very weak chiral response of a generally planar metamaterial severely limits its application. Therefore, it is important to design a system with large circular dichroism. Here we report an optical metamaterial with strong chirality in a bilayer gear-shaped plasmonic structure and consider this chiral response of such fields on tunable atom (87Rb) trapping. Simulation results show that maximum chiral response is observed when the two layers of the gear-shaped structures are rotated from each other by an angle of 60° at λ = 760 nm. Also, we demonstrate an active tunable potential for three-dimensional stable atom-trapping with tunable range of position and potential of a neutral atom of ~58 nm and ~1.3N mK (N denotes the input power with unit mW), respectively. In addition, the trap centers are about hundreds of nanometers away from the structure surface, which ensures the stability of the trapping system. The regulation of neutral atom trapping broadens the application of chiral metamaterials and has potential significance in the manipulation of cold atoms.



Author(s):  
K. Anandan ◽  
V.P. Venkatamuthu

The two types of atoms stable and unstable atoms play the major role in the universe. The space consists of majority of stable atoms in controversy to earth consists of majority of unstable atoms. The attraction and repulsion of unstable atom by stable atom produces a torque. This torque depends on temperature and magnetic field. Thus, the earth rotates about itself. Due to the increase of temperature the diameter of earth increases, that decreases the speed and the spinning of earth; causes climatic change.





Nano Letters ◽  
2008 ◽  
Vol 8 (1) ◽  
pp. 345-349 ◽  
Author(s):  
Makusu Tsutsui ◽  
Kohei Shoji ◽  
Masateru Taniguchi ◽  
Tomoji Kawai


2007 ◽  
Vol 99 (18) ◽  
Author(s):  
Shuai Chen ◽  
Yu-Ao Chen ◽  
Bo Zhao ◽  
Zhen-Sheng Yuan ◽  
Jörg Schmiedmayer ◽  
...  


Author(s):  
Abdul-Wali M. S. Ajlouni

Former studies assumed that, after fission process occurs, the highly ionized new born atoms (20–22 positive charge), ionize the media in which they pass through before becoming stable atoms in a manner similar to 4-MeV-particles. Via ordinary chemical reactions with the surroundings, each stable atom has a probability to form chemical compound. Since there are about 35 different elemental atoms created through fission processes, a large number of chemical species were suggested to be formed. But, these suggested chemical species were not found in the environment after actual releases of FP during accidents like TMI (USA, 1979), and Chernobyl (former USSR, 1986), also the models based on these suggested reactions and species could not interpret the behavior of these actual species. It is assumed here that the ionization states of the new born atoms and the long term high temperature were not dealt with in an appropriate way and they were the reasons of former models failure. Our new approach of DEEP ATOMIC BINDING (DAB) based on the following: 1. The new born atoms which are highly ionized, 10–12 electrons associated with each nucleus, having a large probability to create bonds between them to form molecules. These bonds are at the L, or M shells, and we call it DAB. 2. The molecules stay in the reactor at high temperatures for long periods, so they undergo many stages of composition and decomposition to form giant molecules. By applying DAB approach, field data from Chernobyl, TMI and nuclear detonations could be interpreted with a wide coincidence resulted.



2004 ◽  
Vol 75 (4) ◽  
pp. 1061-1067 ◽  
Author(s):  
Pongpun Rerkkumsup ◽  
Masato Aketagawa ◽  
Koji Takada ◽  
Yoichi Togawa ◽  
Nguyen Tien Thinh ◽  
...  


2004 ◽  
Vol 70 (11) ◽  
pp. 1433-1438
Author(s):  
Yoichi TOGAWA ◽  
Pongpun RERKKUMSUP ◽  
Hiroshi HONDA ◽  
Masato AKETAGAWA ◽  
Koji TAKADA


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