Fiber Coupled Near‐Field Thermoplasmonic Emission from Gold Nanorods at 1100 K

Small ◽  
2021 ◽  
Vol 17 (17) ◽  
pp. 2007274
Author(s):  
Jiayu Li ◽  
Jeffrey Wuenschell ◽  
Zhuo Li ◽  
Subhabrata Bera ◽  
Kai Liu ◽  
...  
Keyword(s):  
2018 ◽  
Vol 124 (2) ◽  
Author(s):  
Kazuharu Uchiyama ◽  
Naoki Nishikawa ◽  
Ryo Nakagomi ◽  
Kiyoshi Kobayashi ◽  
Hirokazu Hori

2015 ◽  
Vol 119 (28) ◽  
pp. 16215-16222 ◽  
Author(s):  
Yoshio Nishiyama ◽  
Keisuke Imaeda ◽  
Kohei Imura ◽  
Hiromi Okamoto

2011 ◽  
Vol 19 (7) ◽  
pp. 6177 ◽  
Author(s):  
E. Boulais ◽  
A. Robitaille ◽  
P. Desjeans-Gauthier ◽  
M. Meunier

2004 ◽  
Vol 108 (42) ◽  
pp. 16344-16347 ◽  
Author(s):  
Kohei Imura ◽  
Tetsuhiko Nagahara ◽  
Hiromi Okamoto

2005 ◽  
Vol 109 (27) ◽  
pp. 13214-13220 ◽  
Author(s):  
Kohei Imura ◽  
Tetsuhiko Nagahara ◽  
Hiromi Okamoto

Author(s):  
Ji-young Kim ◽  
Hsiao-Kuan Yuan ◽  
Reuben M. Bakker ◽  
Vladimir P. Drachev ◽  
Vladimir M. Shalaev
Keyword(s):  

2016 ◽  
Vol 191 ◽  
pp. 9-33 ◽  
Author(s):  
Joshua G. Hinman ◽  
Andrew J. Stork ◽  
Jason A. Varnell ◽  
Andrew A. Gewirth ◽  
Catherine J. Murphy

After a brief review of anisotropy on the nanoscale, experiments in which nanorod core–shell–shell particles are grown are presented. These “nanomatryoshkas” consist of a gold nanorod core, a silica shell, and a final gold shell. Calculation of the near-field properties of these structures using the discrete dipole approximation uncovers the change in location of local electric fields upon gold outer shell growth. Electrochemical experiments of the weak reducing agents used to grow the gold nanorod cores suggest a correlation between the strength of the reducing agent and its ability to promote longer nanorod growth. The final nanostructures do not exhibit a smooth outer shell, unlike their spherical counterparts.


Sign in / Sign up

Export Citation Format

Share Document