Highly efficient and long life metal–insulator–metal cathodes

Author(s):  
Toshiaki Kusunoki ◽  
Mutsumi Suzuki ◽  
Masakazu Sagawa ◽  
Yoshiro Mikami ◽  
Etsuko Nishimura ◽  
...  
2013 ◽  
Vol 1566 ◽  
Author(s):  
Myung-Ki Kim ◽  
Hyuck Choo

ABSTRACTWe demonstrate and analyze a highly efficient on-chip 3D metal-insulator-metal (MIM) nanofocusing structure. Here, we show the in-depth theoretical design, analysis and discussion to provide a detailed picture of the highly efficient, on-chip nanofocusing process which is linearly tapered in 3D.


Plasmonics ◽  
2016 ◽  
Vol 13 (1) ◽  
pp. 141-145 ◽  
Author(s):  
Aliaksandr Hubarevich ◽  
Mikita Marus ◽  
Weijun Fan ◽  
Aliaksandr Smirnov ◽  
Hong Wang

2016 ◽  
Vol 24 (10) ◽  
pp. 10663 ◽  
Author(s):  
Wee Kee Phua ◽  
Yuriy Akimov ◽  
Lin Wu ◽  
Hong Son Chu ◽  
Ping Bai ◽  
...  

ACS Photonics ◽  
2014 ◽  
Vol 1 (10) ◽  
pp. 944-953 ◽  
Author(s):  
Zheng Li ◽  
Jun-long Kou ◽  
Myungki Kim ◽  
Jeong Oen Lee ◽  
Hyuck Choo

2011 ◽  
Author(s):  
Terrance O'Regan ◽  
Matthew Chin ◽  
Cheng Tan ◽  
Anthony Birdwell

2021 ◽  
Vol 11 (4) ◽  
pp. 1544
Author(s):  
Meguya Ryu ◽  
Yoshiaki Nishijima ◽  
Shinya Morimoto ◽  
Naoki To ◽  
Tomoki Hashizume ◽  
...  

The four polarisation method is adopted for measurement of molecular orientation in dielectric nanolayers of metal-insulator-metal (MIM) metamaterials composed of gold nanodisks on polyimide and gold films. Hyperspectral mapping at the chemical finger printing spectral range of 4–20 μμm was carried out for MIM patterns of 1–2.5 μμm period (sub-wavelength). Overlay images taken at 0,π4,π2,3π4 orientation angles and subsequent baseline compensation are shown to be critically important for the interpretation of chemical mapping results and reduction of spurious artefacts. Light field enhancement in the 60-nm-thick polyimide (I in MIM) was responsible for strong absorption at the characteristic polyimide bands. Strong absorbance A at narrow IR bands can be used as a thermal emitter (emittance E=1−R), where R is the reflectance and A=1−R−T, where for optically thick samples the transmittance is T=0.


2021 ◽  
Vol 4 (3) ◽  
pp. 2470-2475 ◽  
Author(s):  
Ayendra Weerakkody ◽  
Amina Belkadi ◽  
Garret Moddel

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