A conjectured explanation for room-temperature superconductivity in narrow channels in oxidized polypropylene

1994 ◽  
Vol 7 (3) ◽  
pp. 679-682 ◽  
Author(s):  
D. M. Eagles
Keyword(s):  
Room Temperature ◽  
Narrow Channels ◽  
Oxidized Polypropylene ◽  
Room Temperature Superconductivity

Bipolaron model of room temperature superconductivity for oxidized polypropylene

2005 ◽  
Vol 722 (1-3) ◽  
pp. 147-149 ◽  
Author(s):  
Liang-You Zheng ◽  
Ying-Nan Chiu ◽  
Shan T. Lai
Keyword(s):  
Room Temperature ◽  
Oxidized Polypropylene ◽  
Room Temperature Superconductivity ◽  
Bipolaron Model

scholarly journals MODIFICATION OF A CHARGED-BOSE-GAS MODEL FOR OBSERVED ROOM-TEMPERATURE SUPERCONDUCTIVITY IN NARROW CHANNELS THROUGH FILMS OF OXIDIZED ATACTIC POLYPROPYLENE

2011 ◽  
Vol 25 (14) ◽  
pp. 1845-1875 ◽  
Author(s):  
D. M. EAGLES
Keyword(s):  
Room Temperature ◽  
Bose Condensation ◽  
Initial Slope ◽  
Atactic Polypropylene ◽  
Minimum Diameter ◽  
Narrow Channels ◽  
Minimum Number ◽  
The One ◽  
Walled Carbon Nanotubes ◽  
Room Temperature Superconductivity

Reasons have been found for thinking that the minimum diameter of channels of a given length to support superconductivity through films of oxidized atactic polypropylene (OAPP) at room temperature is considerably larger than that found in a model for Bose condensation in an array of nanofilaments [D. M. Eagles, Philos. Mag.85, 1931 (2005)] used previously. This model was introduced to interpret experimental results dating from 1988 on OAPP. The channels are thought to be of larger diameter than believed before because, for an N–S–N system where the superconductor consists of an array of single-walled carbon nanotubes, the resistance, for good contacts, is RQ/2N, where N is the number of nanotubes and RQ = 12.9 k Ω [see e.g., M. Ferrier et al., Solid State Commun.131, 615 (2004)]. We assume this would be 2RQ/N for a triplet superconductor with all spins in the same direction and no orbital degeneracy, which may be the case for nanofilaments in OAPP. Hence one may infer a minimum number of filaments for a given resistance. In the present model, the E(K) curve for the bosons is taken to be of a Bogoliubov form, but with a less steep initial linear term in the dispersion at Tc than the one at low T. This form is different from the simple linear plus quadratic dispersion, with a steeper initial slope, used in my 2005 paper. A combination of theory and experimental data has been used to find approximate constraints on parameters appearing in the theory.

On the possibility of room-temperature superconductivity in double stranded DNA

1969 ◽  
Vol 29 (10) ◽  
pp. 636-637 ◽  
Author(s):  
J. Ladik ◽  
A. Bierman
Keyword(s):  
Room Temperature ◽  
Double Stranded Dna ◽  
Room Temperature Superconductivity

Serendipitous vs. systematic search for room-temperature superconductivity

2017 ◽  
Vol 5 (1) ◽  
pp. 161-176 ◽  
Author(s):  
Armen M. Gulian ◽  
Vahan R. Nikoghosyan
Keyword(s):  
Room Temperature ◽  
Systematic Search ◽  
Room Temperature Superconductivity

Vortex Dynamics In case of Possible Room Temperature Superconductivity

2007 ◽  
Author(s):  
Şahin Aktaş ◽  
Selçuk Haciömeroǧlu
Keyword(s):  
Vortex Dynamics ◽  
Room Temperature ◽  
Room Temperature Superconductivity

scholarly journals Microscopic mechanism of room-temperature superconductivity in compressed LaH10

2019 ◽  
Vol 99 (14) ◽  
Author(s):  
Liangliang Liu ◽  
Chongze Wang ◽  
Seho Yi ◽  
Kun Woo Kim ◽  
Jaeyong Kim ◽  
...  
Keyword(s):  
Room Temperature ◽  
Microscopic Mechanism ◽  
Room Temperature Superconductivity
Sign in / Sign up

Export Citation Format

Share Document