Hydroxylated secondary dopants for surface resistance enhancement in transparent poly(3,4-ethylenedioxythiophene)–poly(styrenesulfonate) thin films

2004 ◽  
Vol 142 (1-3) ◽  
pp. 187-193 ◽  
Author(s):  
Brett D Martin ◽  
Nikolay Nikolov ◽  
Steven K Pollack ◽  
Alexey Saprigin ◽  
R Shashidhar ◽  
...  
1997 ◽  
Vol 282-287 ◽  
pp. 591-592 ◽  
Author(s):  
R.X. Wu ◽  
S.Z. Yang ◽  
Y.L. Zhou ◽  
B.B. Jin ◽  
M. Qian ◽  
...  

1988 ◽  
Vol 38 (10) ◽  
pp. 7019-7022 ◽  
Author(s):  
M. S. DiIorio ◽  
Alfredo C. Anderson ◽  
B. -Y. Tsaur

2004 ◽  
Vol 17 (3) ◽  
pp. 337-341 ◽  
Author(s):  
Masashi Mukaida ◽  
Yuya Yamazaki ◽  
Yuki Shingai ◽  
Sayoko Makino ◽  
Masanobu Kusunoki ◽  
...  

2007 ◽  
Vol 21 (18n19) ◽  
pp. 3224-3226
Author(s):  
LIBIN SHI ◽  
YUNFEI WANG ◽  
YUYANG KE ◽  
QUANWU WANG ◽  
ZHEN ZHANG ◽  
...  

The microwave properties of YBa 2 Cu 3 O 7- x / LaAlO 3 (YBCO/LAO) and YBa 2 Cu 3 O 7- x / MgO (YBCO/MgO) thin films have been investigated by microstrip resonator technique. The penetration depth λ0(0 K ) and the microwave surface resistance Rs can be obtained by analyzing the experimental data of the temperature dependence of resonant frequency, unload quality factor of the microstrip resonator. The stress in the two thin films can be obtained from their XRD patterns. The result shows that the stronger stress in YBCO/LAO thing film makes it have larger microwave surface resistance at lower temperature.


2005 ◽  
Vol 15 (2) ◽  
pp. 3692-3695 ◽  
Author(s):  
A. Saito ◽  
M. Shirakawa ◽  
K. Kitamura ◽  
Y. Noguchi ◽  
M. Mukaida ◽  
...  

1991 ◽  
Vol 6 (11) ◽  
pp. 2259-2263 ◽  
Author(s):  
K.H. Young ◽  
McD. Robinson ◽  
G.V. Negrete ◽  
T. Yamashita ◽  
T. Hirai ◽  
...  

The microstructure and microwave properties of YBa2Cu3O7−δ thin films grown on SrTiO3 (100) and MgO (100) substrates by chemical vapor deposition have been studied. Both 100 GHz cavity measurement of surface resistance and ground plane substitution in a 5 GHz microstrip resonator show that films on SrTiO3 have better microwave properties than those on MgO. Although there are some a-axis grains and secondary phases on the surface, a large fraction of each film on SrTiO3 is epitaxial with its c axis normal to the substrate. The 100 GHz surface resistance of these films is less than copper for temperature ⋚ 82 K, and approaches the detection limit at 10–20 K. For the films on MgO, c-axis grains of different in-plane rotation are found together with some a-axis needle-like grains. The grain boundaries are detrimental to the microwave properties, and the resulting surface resistance at 100 GHz and 10–20 K is about 20 mΩ higher than that of films on SrTiO3.


2004 ◽  
Vol 96 (11) ◽  
pp. 6527-6533 ◽  
Author(s):  
M. Murugesan ◽  
H. Obara ◽  
S. Kosaka ◽  
H. Yamasaki ◽  
B. Prijamboedi

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